čipový

čipový (masculine nominative singular)
čipová (feminine nominative singular)
čipové (neuter nominative singular)
čipového (genitive masculine singular)
čipové (feminine genitive singular)
čipového (genitive neuter singular)
čipovému (dative masculine singular)
čipové (dative feminine singular)
čipovému (dative neuter singular)
čipového (accusative animate masculine singular)
čipový (accusative inanimate masculine singular)
čipovou (accusative feminine singular)
čipové (accusative neuter singular)
čipovém (locative masculine singular)
čipové (feminine locative singular)
čipovém (locative neuter singular)
čipovým (instrumental masculine singular)
čipovou (feminine instrumental singular)
čipovým (instrumental neuter singular)
čipoví (animate masculine nominative plural)
čipové (feminine nominative plural)
čipové (inanimate masculine nominative plural)
čipová (neuter nominative plural)
čipových (genitive plural)
čipovým (dative plural)
čipové (accusative feminine masculine plural)
čipová (accusative neuter plural)
čipových (locative plural)
čipovými (instrumental plural)


light minute

Rick: We got some business to attend to a few light minutes south of here.

2015, "Mortynight Run", season 2, episode 2 of Rick and Morty [Rick and Morty are travelling in a spaceship]

(astronomy, physics) A unit of length equal to the distance light travels in one minute.


hyperonization

A possibility of hyperonization of the matter in neutron star interiors is incorporated.

2015, K.A. Maslov, E.E. Kolomeitsev, D.N. Voskresensky, “Relativistic Mean-Field Models with Scaled Hadron Masses and Couplings: Hyperons and Maximum Neutron Star Mass”, in arXiv:

(physics) Conversion to, or consideration as hyperons


superrenormalizable

LL-Q1860 (eng)-Flame, not lame-superrenormalizable.wav

Our proof is somewhat nontrivial, suggesting that there may be alternative formulations of quantum field theory that make the QNEC more manifest. Our proof applies to free and superrenormalizable bosonic field theories, and to any points that lie on stationary null surfaces.

2015, Raphael Bousso, Zachary Fisher, Jason Koeller, Stefan Leichenauer, Aron C. Wall, “Proof of the Quantum Null Energy Condition”, in arXiv:


晶粒

/t͡ɕiŋ⁵⁵ li⁵¹/

/t͡ɕiŋ⁵⁵ liə̯ɻ⁵¹/

/t͡sɪŋ⁵⁵ nɐp̚⁵/

/t͡sɪŋ⁵⁵ lɐp̚⁵/

/t͡ɕiŋ⁵⁵ li⁵¹/

/t͡ɕiŋ⁵⁵ liə̯ɻ⁵¹/

/t͡sɪŋ⁵⁵ nɐp̚⁵/

/t͡sɪŋ⁵⁵ lɐp̚⁵/

(electronics) die (small block of semiconducting material on which a given functional circuit is fabricated)


anodiparisto

anodiparisto (nominative singular)
anodiparistot (nominative plural)
anodiparisto (accusative nominative singular)
anodiparistot (accusative nominative plural)
anodipariston (accusative genitive singular)
anodiparistot (accusative genitive plural)
anodipariston (genitive singular)
anodiparistojen (genitive plural)
anodiparistoiden (genitive plural)
anodiparistoitten (genitive plural)
anodiparistoa (partitive singular)
anodiparistoja (partitive plural)
anodiparistoita (partitive plural)
anodiparistossa (inessive singular)
anodiparistoissa (inessive plural)
anodiparistosta (elative singular)
anodiparistoista (elative plural)
anodiparistoon (illative singular)
anodiparistoihin (illative plural)
anodiparistolla (adessive singular)
anodiparistoilla (adessive plural)
anodiparistolta (ablative singular)
anodiparistoilta (ablative plural)
anodiparistolle (allative singular)
anodiparistoille (allative plural)
anodiparistona (essive singular)
anodiparistoina (essive plural)
anodiparistoksi (singular translative)
anodiparistoiksi (plural translative)
anodiparistotta (abessive singular)
anodiparistoitta (abessive plural)
anodiparistoin (instructive plural)
See the possessive forms below. (comitative)
anodiparistoni (nominative singular)
anodiparistoni (nominative plural)
anodiparistoni (accusative nominative singular)
anodiparistoni (accusative nominative plural)
anodiparistoni (accusative genitive singular)
anodiparistoni (accusative genitive plural)
anodiparistoni (genitive singular)
anodiparistojeni (genitive plural)
anodiparistoideni (genitive plural)
anodiparistoitteni (genitive plural)
anodiparistoani (partitive singular)
anodiparistojani (partitive plural)
anodiparistoitani (partitive plural)
anodiparistossani (inessive singular)
anodiparistoissani (inessive plural)
anodiparistostani (elative singular)
anodiparistoistani (elative plural)
anodiparistooni (illative singular)
anodiparistoihini (illative plural)
anodiparistollani (adessive singular)
anodiparistoillani (adessive plural)
anodiparistoltani (ablative singular)
anodiparistoiltani (ablative plural)
anodiparistolleni (allative singular)
anodiparistoilleni (allative plural)
anodiparistonani (essive singular)
anodiparistoinani (essive plural)
anodiparistokseni (singular translative)
anodiparistoikseni (plural translative)
anodiparistottani (abessive singular)
anodiparistoittani (abessive plural)
anodiparistoineni (comitative plural)
anodiparistosi (nominative singular)
anodiparistosi (nominative plural)
anodiparistosi (accusative nominative singular)
anodiparistosi (accusative nominative plural)
anodiparistosi (accusative genitive singular)
anodiparistosi (accusative genitive plural)
anodiparistosi (genitive singular)
anodiparistojesi (genitive plural)
anodiparistoidesi (genitive plural)
anodiparistoittesi (genitive plural)
anodiparistoasi (partitive singular)
anodiparistojasi (partitive plural)
anodiparistoitasi (partitive plural)
anodiparistossasi (inessive singular)
anodiparistoissasi (inessive plural)
anodiparistostasi (elative singular)
anodiparistoistasi (elative plural)
anodiparistoosi (illative singular)
anodiparistoihisi (illative plural)
anodiparistollasi (adessive singular)
anodiparistoillasi (adessive plural)
anodiparistoltasi (ablative singular)
anodiparistoiltasi (ablative plural)
anodiparistollesi (allative singular)
anodiparistoillesi (allative plural)
anodiparistonasi (essive singular)
anodiparistoinasi (essive plural)
anodiparistoksesi (singular translative)
anodiparistoiksesi (plural translative)
anodiparistottasi (abessive singular)
anodiparistoittasi (abessive plural)
anodiparistoinesi (comitative plural)
anodiparistomme (nominative singular)
anodiparistomme (nominative plural)
anodiparistomme (accusative nominative singular)
anodiparistomme (accusative nominative plural)
anodiparistomme (accusative genitive singular)
anodiparistomme (accusative genitive plural)
anodiparistomme (genitive singular)
anodiparistojemme (genitive plural)
anodiparistoidemme (genitive plural)
anodiparistoittemme (genitive plural)
anodiparistoamme (partitive singular)
anodiparistojamme (partitive plural)
anodiparistoitamme (partitive plural)
anodiparistossamme (inessive singular)
anodiparistoissamme (inessive plural)
anodiparistostamme (elative singular)
anodiparistoistamme (elative plural)
anodiparistoomme (illative singular)
anodiparistoihimme (illative plural)
anodiparistollamme (adessive singular)
anodiparistoillamme (adessive plural)
anodiparistoltamme (ablative singular)
anodiparistoiltamme (ablative plural)
anodiparistollemme (allative singular)
anodiparistoillemme (allative plural)
anodiparistonamme (essive singular)
anodiparistoinamme (essive plural)
anodiparistoksemme (singular translative)
anodiparistoiksemme (plural translative)
anodiparistottamme (abessive singular)
anodiparistoittamme (abessive plural)
anodiparistoinemme (comitative plural)
anodiparistonne (nominative singular)
anodiparistonne (nominative plural)
anodiparistonne (accusative nominative singular)
anodiparistonne (accusative nominative plural)
anodiparistonne (accusative genitive singular)
anodiparistonne (accusative genitive plural)
anodiparistonne (genitive singular)
anodiparistojenne (genitive plural)
anodiparistoidenne (genitive plural)
anodiparistoittenne (genitive plural)
anodiparistoanne (partitive singular)
anodiparistojanne (partitive plural)
anodiparistoitanne (partitive plural)
anodiparistossanne (inessive singular)
anodiparistoissanne (inessive plural)
anodiparistostanne (elative singular)
anodiparistoistanne (elative plural)
anodiparistoonne (illative singular)
anodiparistoihinne (illative plural)
anodiparistollanne (adessive singular)
anodiparistoillanne (adessive plural)
anodiparistoltanne (ablative singular)
anodiparistoiltanne (ablative plural)
anodiparistollenne (allative singular)
anodiparistoillenne (allative plural)
anodiparistonanne (essive singular)
anodiparistoinanne (essive plural)
anodiparistoksenne (singular translative)
anodiparistoiksenne (plural translative)
anodiparistottanne (abessive singular)
anodiparistoittanne (abessive plural)
anodiparistoinenne (comitative plural)
anodiparistonsa (nominative singular)
anodiparistonsa (nominative plural)
anodiparistonsa (accusative nominative singular)
anodiparistonsa (accusative nominative plural)
anodiparistonsa (accusative genitive singular)
anodiparistonsa (accusative genitive plural)
anodiparistonsa (genitive singular)
anodiparistojensa (genitive plural)
anodiparistoidensa (genitive plural)
anodiparistoittensa (genitive plural)
anodiparistoaan (partitive singular)
anodiparistoansa (partitive singular)
anodiparistojaan (partitive plural)
anodiparistoitaan (partitive plural)
anodiparistojansa (partitive plural)
anodiparistoitansa (partitive plural)
anodiparistossaan (inessive singular)
anodiparistossansa (inessive singular)
anodiparistoissaan (inessive plural)
anodiparistoissansa (inessive plural)
anodiparistostaan (elative singular)
anodiparistostansa (elative singular)
anodiparistoistaan (elative plural)
anodiparistoistansa (elative plural)
anodiparistoonsa (illative singular)
anodiparistoihinsa (illative plural)
anodiparistollaan (adessive singular)
anodiparistollansa (adessive singular)
anodiparistoillaan (adessive plural)
anodiparistoillansa (adessive plural)
anodiparistoltaan (ablative singular)
anodiparistoltansa (ablative singular)
anodiparistoiltaan (ablative plural)
anodiparistoiltansa (ablative plural)
anodiparistolleen (allative singular)
anodiparistollensa (allative singular)
anodiparistoilleen (allative plural)
anodiparistoillensa (allative plural)
anodiparistonaan (essive singular)
anodiparistonansa (essive singular)
anodiparistoinaan (essive plural)
anodiparistoinansa (essive plural)
anodiparistokseen (singular translative)
anodiparistoksensa (singular translative)
anodiparistoikseen (plural translative)
anodiparistoiksensa (plural translative)
anodiparistottaan (abessive singular)
anodiparistottansa (abessive singular)
anodiparistoittaan (abessive plural)
anodiparistoittansa (abessive plural)
anodiparistoineen (comitative plural)
anodiparistoinensa (comitative plural)

anodi + paristo; calque of German Anodenbatterie (“B battery”)

cal

(electronics) B battery (battery used to provide the plate voltage for a vacuum tube)


B battery

(dated, electronics) A battery used to provide the plate voltage for a vacuum tube.


負載

/fu⁵¹⁻⁵³ t͡saɪ̯⁵¹/

/fuː²² t͡sɔːi̯³³/

/hu⁴¹⁻⁵⁵⁴ t͡sai⁴¹/

/hu²²⁻²¹ t͡sai²¹/

/hu³³⁻²¹ t͡sai²¹/

/hu³³⁻¹¹ t͡sai¹¹/

/fu⁵¹⁻⁵³ t͡saɪ̯⁵¹/

/fuː²² t͡sɔːi̯³³/

/hu⁴¹⁻⁵⁵⁴ t͡sai⁴¹/

/hu²²⁻²¹ t͡sai²¹/

/hu³³⁻²¹ t͡sai²¹/

/hu³³⁻¹¹ t͡sai¹¹/


violetward

en-adj

violetward (comparative more violetward, superlative most violetward)

more violetward (comparative)
most violetward (superlative)

(physics) Toward the violet end of the spectrum.


plexciton

(physics) A polaritonic mode that results from the strong coupling between excitons and plasmons


hyperconductor

In this paper, we compute the low-temperature DC and AC electrical and thermal conductivities in a one-dimensional hyperconductor, studied previously by the present authors, in the presence of both disorder and umklapp scattering.

2015, Eugeniu Plamadeala, Michael Mulligan, Chetan Nayak, “Transport in a One-Dimensional Hyperconductor”, in arXiv:

(physics) A superconductor that also has infinite thermal conductivity (at zero temperature)


magnetofluidodynamic

Our predictions are based on estimating 3D corrections to a simple, yet powerful plane magnetofluidodynamic model where the equations to be solved are reduced to a system of Hamilton equations in one dimension (or a collection of) which become autonomous after the pulse has overcome the electrons.

2015, Gaetano Fiore, Sergio De Nicola, “A simple model of the slingshot effect”, in arXiv:

(physics) Relating to magnetofluidodynamics


magnetofluidodynamics

(physics) An extension of magnetohydrodynamics to cover fluids other than water


equiconvex

equiconvex (comparative more equiconvex, superlative most equiconvex)

more equiconvex (comparative)
most equiconvex (superlative)

(optics, of a lens) Having surfaces with the same convex radius of curvature.


enhancon

Instead, we show how to construct reliable sugra duals to particular points on the Coulomb branch where the enhancon is screened.

2015, William Cottrell, James Hanson, Akikazu Hashimoto, “Dynamics of cal N=4 supersymmetric field theories in 2+1 dimensions and their gravity dual”, in arXiv:

(mathematics, physics) A type of conifold ring proposed in some forms of supersymmetry.


repulson

We find that the gravity duals of theories with klt;(N-M) contain enhancons even in situations where repulson singularities are absent.

(physics) A repulsive singularity proposed in some forms of gauge theory


skyrmionics

In this paper we explore topologically protected magnetic solitons that might potentially be applied for logical operations and/or information storage in the rapidly advancing field of solitonics (and skyrmionics).

2015, Konstantinos Koumpouras, Anders Bergman, Olle Eriksson, Dmitry Yudin, “A spin dynamics approach to solitonics”, in arXiv:


tyngdefelt

tyngdefelt (indefinite nominative singular)
tyngdefeltet (definite nominative singular)
tyngdefelter (indefinite nominative plural)
tyngdefelterne (definite nominative plural)
tyngdefelts (genitive indefinite singular)
tyngdefeltets (definite genitive singular)
tyngdefelters (genitive indefinite plural)
tyngdefelternes (definite genitive plural)


spherocylindrical

spherocylindrical (comparative more spherocylindrical, superlative most spherocylindrical)

more spherocylindrical (comparative)
most spherocylindrical (superlative)

From sphere + o + cylindrical or spherocylinder + -ical.

(optics, of a lens) Having one spheric and one cylindric surface.


anticonvective

anticonvective (comparative more anticonvective, superlative most anticonvective)

more anticonvective (comparative)
most anticonvective (superlative)


保真

/pɑʊ̯²¹⁴⁻²¹ ʈ͡ʂən⁵⁵/

/pɑʊ̯²¹⁴⁻²¹ ʈ͡ʂən⁵⁵/


hyperfragment

(physics) A very short-lived hyperonic fragment of a stable nuclide


nonbond

Compression shortens the O:H nonbond and lengthens the H-O bond simultaneously via O:H-O Coulomb repulsion.

2015, Chang Q. Sun, “Why does pressure melt ice?”, in arXiv:

(chemistry, physics) A nonbonding relationship between two atoms


ttbar

The cross section for ttbar production in the all-jets final state is measured in pp collisions at a centre-of-mass energy of 8 TeV at the LHC with the CMS detector, in data corresponding to an integrated luminosity of 18.4 inverse femtobarns.

2015, CMS Collaboration, “Measurement of the ttbar production cross section in the all-jets final state in pp collisions at sqrt(s)=8 TeV”, in arXiv:

(physics) A top quark and top antiquark pair of particles


ultrastatic

We adopt a Faddeev-Jackiw method of quantization and consider the case of an ultrastatic spacetime for simplicity.

2015, David J. Toms, “Quantization of the minimal and non-minimal vector field in curved space”, in arXiv:

(physics, of a spacetime) static in a precisely defined way


polarizance

en-noun

polarizance (countable and uncountable, plural polarizances)

Am A 13, 1106 (1996)] any depolarizing Mueller matrix can be transformed into a reduced form which accumulates the depolarization and polarizance properties into a set of seven parameters.

2015, Jose J. Gil, Ignacio San Jose, “Reduced form of a Mueller matrix”, in arXiv:

(physics) The ability to produce polarized light


taudeeltje

Compound of tau (“Greek letter tau”) + deeltje (“particle”).


magnetoshear

We find evidence for the action of a non-axisymmetric magnetoshear instability operating in the upper portions of the stably stratified fluid layers.

2015, N. Lawson, A. Strugarek, P. Charbonneau, “Evidence of active MHD instability in EULAG-MHD simulations of solar convection”, in arXiv:


underbarrier

LL-Q1860 (eng)-Flame, not lame-underbarrier.wav

Initial conditions for inflation are set up by cosmological instantons describing underbarrier oscillations in the vicinity of the inflaton potential maximum.

2015, A.O. Barvinsky, A.Yu. Kamenshchik, “New type of hill-top inflation: CFT driven cosmology”, in arXiv:


anticoherence

We provide three different characterizations of anticoherence, and establish a link between symmetries, anticoherence and classes of states equivalent through stochastic local operations with classical communication (SLOCC).

2015, D. Baguette, F. Damanet, O. Giraud, J. Martin, “Anticoherence of spin states with point group symmetries”, in arXiv:

(physics) The condition of being anticoherent


anticoherent

(physics, of waves etc) Having the same wavelength and phase but the opposite direction


antiferroquadrupolar

No explicit sign of time-reversal symmetry breaking was found below the multipolar order temperature T#95;Q#92;sim 0.6 K in a zero applied field as anticipated on the basis of the antiferroquadrupolar (AFQ) order picture proposed by Sakai and Nakatsuji [J.

2015, T. U. Ito, W. Higemoto, A. Sakai, M. Tsujimoto, S. Nakatsuji, “Perturbation on Hyperfine-enhanced ¹⁴¹Pr Nuclear Spin Dynamics Associated with Antiferroquadrupolar Order in PrV₂Al₂₀”, in arXiv:

(physics) antiferromagnetic and quadrupolar


induksjonsmotor

induksjonsmotoren (definite singular)
induksjonsmotorer (indefinite plural)
induksjonsmotorene (definite plural)


induksjonsmotor

induksjonsmotoren (definite singular)
induksjonsmotorar (indefinite plural)
induksjonsmotorane (definite plural)


pbar

(physics) antiproton (pronunciation spelling of the symbol p̄)


pionful

By reviewing the transition from one effective field theory to another, from QCD to pionful chiral theories to pionless and eventually to cluster theories, we identify some of those deficiencies and conceptual problems awaiting a solution before QCD can be identified as the high-energy theory from which the nuclear landscape emerges..

2015, Johannes Kirscher, “Matching effective few-nucleon theories to QCD”, in arXiv:

(physics, of a theory) That includes pions


quasiparton

Recent developments showed that light cone parton distributions can be studied by investigating the large momentum limit of the so-called quasiparton distributions, which are defined in terms of spacelike correlators, and therefore can be readily computed on the lattice.

2015, Xiaonu Xiong, Jian-Hui Zhang, “One-loop matching for transversity generalized parton distribution”, in arXiv:


triboson

I summarize an extensive ATLAS and CMS electroweak physics program that involves a variety of single boson, diboson, triboson, and vector boson scattering measurements.

2015, Junjie Zhu, “Electroweak results from the ATLAS and CMS experiments”, in arXiv:

(physics) Any particle composed of three bosons


undvigelseshastighed

undvigelseshastighed (indefinite nominative singular)
undvigelseshastigheden (definite nominative singular)
undvigelseshastigheder (indefinite nominative plural)
undvigelseshastighederne (definite nominative plural)
undvigelseshastigheds (genitive indefinite singular)
undvigelseshastighedens (definite genitive singular)
undvigelseshastigheders (genitive indefinite plural)
undvigelseshastighedernes (definite genitive plural)

Undvigelseshastigheden for et projektil fra en planet er kvadratroden af 2 gange planetens masse gange gravitationskonstanten divideret med planetens radius.

The escape velocity for a projectile from a planet is the square root of 2 times the mass of the planet times the gravitation constant divided by the radius of the planet.


three-phase

By the end of the year all new electrification projects were virtually complete and conversion of the remaining three-phase 3,700V a.c. sections to 3,000V d.c. was well in hand.

1963 January, “Beyond the Channel: Italy”, in Modern Railways, page 62:

(electricity) Using three separate alternating currents of the same voltage at different phases.

трифазен

using three separate alternating currents


gluónico

pt-adj

gluónico (feminine gluónica, masculine plural gluónicos, feminine plural gluónicas, not comparable)

gluónica (feminine)
gluónicos (masculine plural)
gluónicas (feminine plural)


gluónico

es-adj

gluónico (feminine gluónica, masculine plural gluónicos, feminine plural gluónicas)


發光二極管

ㄈㄚ ㄍㄨㄤ ㄦˋ ㄐㄧˊ ㄍㄨㄢˇ

фагуан эрцзигуань

/fä⁵⁵ ku̯ɑŋ⁵⁵ ˀɤɻ⁵¹ t͡ɕi³⁵ ku̯än²¹⁴⁻²¹⁽⁴⁾/

ㄈㄚ ㄍㄨㄤ ㄦˋ ㄐㄧˊ ㄍㄨㄢˇㄦ

фагуанъэрцзигуаньр

/fä⁵⁵ ku̯ɑŋ⁵⁵ ˀɤɻ⁵¹ t͡ɕi³⁵ ku̯ɑɻ²¹⁴⁻²¹⁽⁴⁾/

/faːt̚³ kʷɔːŋ⁵⁵ jiː²² kɪk̚² kuːn³⁵/

/faːt̚³ kʷɔːŋ⁵⁵ jiː²² kɪk̚² kuːn³⁵/

light-emitting diode
light-emitting diode


磁層

/t͡sʰz̩³⁵ t͡sʰɤŋ³⁵/

/t͡sʰiː²¹ t͡sʰɐŋ²¹/

/t͡sʰz̩³⁵ t͡sʰɤŋ³⁵/

/t͡sʰiː²¹ t͡sʰɐŋ²¹/


壓力計

/jä⁵⁵ li⁵¹⁻⁵³ t͡ɕi⁵¹/

/aːt̚³ lɪk̚² kɐi̯³³/

/jä⁵⁵ li⁵¹⁻⁵³ t͡ɕi⁵¹/

/aːt̚³ lɪk̚² kɐi̯³³/


supermomentum

LL-Q1860 (eng)-Flame, not lame-supermomentum.wav

The supermomentum charges are associated with ordinary gravitational wave memory, and the super center-of-mass charges are associated with total (ordinary plus null) gravitational wave memory, in the terminology of Bieri and Garfinkle.

2015, Eanna E. Flanagan, David A. Nichols, “Conserved charges of the extended Bondi-Metzner-Sachs group”, in arXiv:


thermalon

The geometric conditions based on the properties of free thermalon solutions that are proposed for conversion to a high temperature hologram to occur, however, are local and generic in dimension and could apply throughout M space.

2015, Michael Hewitt, “String condensation: Nemesis of Black Holes?”, in arXiv:

(physics) A pseudoparticle associated with the thermal properties of the event horizon of a black hole


diquarkonium

In this note we attempt an estimate of its transition rate through a non-relativistic calculation of the electric dipole term of a diquarkonium bound state.

2015, H.-X. Chen, L. Maiani, A.D. Polosa, V. Riquer, “Y(4260) --> gamma + X(3872) in the diquarkonium picture”, in arXiv:

(physics) A metastable state formed from a pair of diquarks


hyperhelium

Using the coalescence model based on the phase-space distributions of protons, neutrons, Lambdas and their antiparticles from a multiphase transport (AMPT) model, we study the production of deuteron, triton, helium 3, hypertriton, hyperhelium 3 and their antinuclei in Pb+Pb collisions at #92;sqrt#123;s#95;#123;NN

2015, Lilin Zhu, Che Ming Ko, Xuejiao Yin, “Light (anti-)nuclei production and flow in relativistic heavy-ion collisions”, in arXiv:

(physics) A nuclear complex formed from a helium nucleus by replacement of a neutron by a hyperon


核裂變

ㄏㄜˊ ㄌㄧㄝˋ ㄅㄧㄢˋ

/xɤ³⁵ li̯ɛ⁵¹⁻⁵³ pi̯ɛn⁵¹/

/xɤ³⁵ li̯ɛ⁵¹⁻⁵³ pi̯ɛn⁵¹/


核聚變

ㄏㄜˊ ㄐㄩˋ ㄅㄧㄢˋ

/xɤ³⁵ t͡ɕy⁵¹⁻⁵³ pi̯ɛn⁵¹/

/hɐt̚² t͡sɵy̯²² piːn³³/

/xɤ³⁵ t͡ɕy⁵¹⁻⁵³ pi̯ɛn⁵¹/

/hɐt̚² t͡sɵy̯²² piːn³³/


裂變

/li̯ɛ⁵¹⁻⁵³ pi̯ɛn⁵¹/

/li̯ɛ⁵¹⁻⁵³ pi̯ɛn⁵¹/


sbar

No significant deviation is observed in the data with respect to the standard model predictions, and model-independent upper limits are set on the branching fraction BF( t to H+ b ), ranging from 1.2 to 6.5% for a charged Higgs boson with mass between 90 and 160 GeV, under the assumption that BF( H+ to c sbar ) = 100%..

2015, CMS Collaboration, “Search for a light charged Higgs boson decaying to c-sbar in pp collisions at sqrt(s) = 8 TeV”, in arXiv:

anti-strange quark
anti-strange quark#English

(physics) Abbreviation of anti-strange quark.


bandlimit

We conclude that, either superoscillations really can beat the bandlimit and achieve superresolution (`kinematic superresolution') or the superoscillating high frequency is absorbed and we gain dynamical access to the physics of high frequency processes with low frequency signals (`dynamical superresolution')..

2015, Achim Kempf, Angus Prain, “Driving Quantum Systems with Superoscillations”, in arXiv:

(physics) The limiting frequency of a signal beyond which the intensity of the signal is zero


itinerance

Their precise role in the interplay between itinerance and localisation, long known to underpin Mottness in d-band oxides, has however received much less attention.

2015, Mukul S. Laad, S. Koley, A. Taraphder, “Mott transitions and Novel Orders in Multi-Orbital Models: The Relevance of Structural "Double Exchange"”, in arXiv:

(physics) The (often chaotic) movement of electrons through a material


superoscillating

LL-Q1860 (eng)-Flame, not lame-superoscillating.wav


crosswedge

For this asymptotic case we are considering, k - r \, and * - (54), is the distance from the apex multiplied by some constant factor Fig 4 shows that the crosswedge wavelength decreases as the wave approaches the apex.

1982, Woods Hole Oceanographic Institution, Collected Reprints - Issue 2, page 867:

Thus analytical surface wave solutions are available to describe waves that are either progressive or trapped in the crosswedge direction.

2012, A. R. Robinson, Eddies in Marine Science, →ISBN:

The test calculations are carried out for the crosswedge benchmark and proved an excellent agreement with the source images method.

2015, M.Yu. Trofimov, A.D. Zakharenko, S.B. Kozitskiy, “Mode Gaussian beam tracing”, in arXiv:

(physics) A wedge-shaped waveform that moves in the cross direction to the current.


geofizician

ro-noun

geofizician m (plural geofizicieni, feminine equivalent geofiziciană)

geofizicieni (plural)
equivalent geofiziciană (feminine)
geofizician (accusative indefinite nominative singular)
geofizicianul (accusative definite nominative singular)
geofizicieni (accusative indefinite nominative singular)
geofizicienii (accusative definite nominative plural)
geofizician (indefinite singular)
geofizicianului (definite singular)
geofizicieni (indefinite singular)
geofizicienilor (definite plural)
geofizicianule (singular vocative)
geofizicienilor (vocative)


mesoglass

(physics) A glass (especially a spin glass) whose properties are evident on a mesoscopic scale


metamolecule

By means of breaking the geometric symmetry of the metamolecule, the toroidal mode can be excited by linearly polarized light and we provide simple optimization protocols for maximizing the toroidal dipole mode excitation.

2015, Derek W. Watson, Stewart D. Jenkins, Janne Ruostekoski, Vassili A. Fedotov, Nikolay I. Zheludev, “Toroidal dipole excitations in metamolecules formed by interacting plasmonic nanorods”, in arXiv:

(physics) A grouping of atoms held together by a magnetic field rather than by interatomic forces


photoreflectance

We observe a pronounced dependency of the quality factor on the measurement scheme, and find that significantly larger quality factors can be extracted in photoreflectance compared to photoluminescence measurements.

2015, Christian Schneider, Peter Gold, Stephan Reitzenstein, Sven Hoefling, Martin Kamp, “Quantum dot micropillar cavities with quality factors exceeding 250,000”, in arXiv:

(physics) reflectance that varies according to the incident light level


skewon

The identity of Fresnel and Kummer surfaces, which holds true for media with a certain symmetry (zero skewon piece), provides an elegant interpretation of the results.

2015, Alberto Favaro, Friedrich W. Hehl, “Light propagation in local and linear media: Fresnel-Kummer wave surfaces with 16 singular points”, in arXiv:

(physics) A theoretical particle related to the axion and dilaton


inductionless

We consider the nonaxisymmetric modes of instability present in Taylor-Couette flow under the application of helical magnetic fields, mainly for magnetic Prandtl numbers close to the inductionless limit, and conduct a full examination of marginal stability in the resulting parameter space.

2015, Adam Child, Evy Kersalé, Rainer Hollerbach, “Nonaxisymmetric linear instability of cylindrical magnetohydrodynamic Taylor-Couette flow”, in Physical Review E, volume 92:


subvacuum

en-noun

subvacuum (plural subvacuums or subvacua)

It is found possible for this decoherence to be below the level from the pure vacuum, rendering another subvacuum phenomenon of recoherence.

2015, Chen-Pin Yeh, Da-Shin Lee, “Subvacuum effects in Quantum Critical Theories from Holographic Approach”, in arXiv:

(physics) A quantum field or spacetime obtained from a vacuum by a "squeezing" process


Tx

Alternative form: tx

(uncountable, electronics, telecommunications) Abbreviation of transmission.


引力相互作用

ㄧㄣˇ ㄌㄧˋ ㄒㄧㄤ ㄏㄨˋ ㄗㄨㄛˋ ㄩㄥˋ

иньли сянху цзоюн

/in²¹⁴⁻²¹ li⁵¹ ɕi̯ɑŋ⁵⁵ xu⁵¹⁻⁵³ t͡su̯ɔ⁵¹⁻⁵³ jʊŋ⁵¹/

gravitational interaction
gravitational interaction


eigenstrain

Optimal structures are either simple laminates that are codirected with external eigenstrain directions, or inclined laminates, direct and skew second-rank laminates and third-rank laminates.

2015, Mikhail A. Antimonov, Andrej Cherkaev, Alexander Freidin, “Phase transformations surfaces and exact energy lower bounds”, in arXiv:

(physics) A residual strain produced without an external force


eigenstress

(physics) A stress produced by an eigenstrain


superfocusing

LL-Q1860 (eng)-Flame, not lame-superfocusing.wav

We theoretically demonstrate the possibility of controlling nanoscale short pulse superfocusing based on the generation of radially polarized surface plasmon polariton mode of conical metallic tip.

2015, P.A. Golovinski, V.A. Astapenko, E.S. Manuylovich, “Diffraction of Ultrashort Pulse on a Nanoscale Conductive Cone”, in arXiv:

(physics) focusing at wavelengths greater than is possible using diffraction


ferrielectric

transition temperature
transition temperature

(physics) antiferroelectric with a transition temperature to another form


optomagnonics

An understanding of the magneto-optical coupling in whispering gallery modes, where the propagation direction rotates with respect to the magnetization, is fundamental to the emerging field of cavity optomagnonics..

2015, J. A. Haigh, S. Langenfeld, N. J. Lambert, J. J. Baumberg, A. J. Ramsay, A. Nunnenkamp, A. J. Ferguson, “Magneto-optical coupling in whispering gallery mode resonators”, in arXiv:


photoenergy

photoenergy (countable and uncountable, plural photoenergies)

For photoexcited molecules, the nuclear dynamics determine the photoenergy conversion path and efficiency.

2015, Jie Yang, Markus Guehr, Theodore Vecchione, Matthew S. Robinson, Renkai Li, Nick Hartmann, Xiaozhe Shen, Ryan Coffee, Jeff Corbett, Alan Fry, Kelly Gaffney, Tais Gorkhover, Carsten Hast, Keith Jobe, Igor Makasyuk, Alexander Reid, Joseph Robinson, Sharon Vetter, Fenglin Wang, Stephen Weathersby, Charles Yoneda, Martin Centurion, Xijie Wang, “Diffractive imaging of a molecular rotational wavepacket with femtosecond Megaelectronvolt electron pulses”, in arXiv:

(physics) The energy of a system of photons or other wavepackets


hyperconductivity

These novel phenomena and applications include super resolution imaging, new stealth technologies, enhanced quantum-electrodynamic effects, thermal hyperconductivity, superconductivity, and interesting gravitation theory analogues.

2015, Igor I. Smolyaninov, “Hyperbolic Metamaterials”, in arXiv:

(physics) The condition of being hyperconductive


polyfold

Each group of lines may be accounted for by transitions of the valence electron between a polyfold level of one type and another polyfold level of the same or different type.

1925, Scientific papers of the Bureau of Standards - Volume 19, page 121:

Multiplicities of the energy states of the polyfold spectral terms depend on the valence electrons of the atoms.

1926, Herbert Treadwell Wade, The New International Year Book, page 557:

These levels comprise the components of spectral terms which are usually polyfold, but it is sometimes difficult or impossible without Zeeman effects or similar criteria to fix the absolute values of the quantum numbers which define the types

1928, Optical society of America - Volume 17, page 84:

Sommerfeld invented " inner quantum numbers " to distinguish the levels of polyfold spectral terms.

1990, Commentarium Scientificum Internationale Tractans de Re Spectrochimica:

(physics) Having the same total and azimuthal quantum numbers, similar energy values, but different inner quantum numbers.


synchronverter

This paper sketches the ideas of a viable alternative for traditional remedial controls for power grids with high penetration of renewables, in which the renewables are integrated with synchronverters to mimic the dynamics of conventional generators.

2015, Thanh Long Vu, Spyros Chatzivasileiadis, Konstantin Turitsyn, “Towards Electronics-based Emergency Control in Power Grids with High Renewable Penetration”, in arXiv:


pseudomagnetic

LL-Q1860 (eng)-Flame, not lame-pseudomagnetic.wav

Numerical tight binding calculations of single pseudomagnetic dots in extended graphene sheets confirm these predictions, and are also used to study the effect of the rotating the strain direction and varying the size of the pseudomagnetic dot..

2015, Mikkel Settnes, Stephen R. Power, Antti-Pekka Jauho, “Pseudomagnetic fields and triaxial strain in graphene”, in arXiv:

(physics) That interacts with an electric field in a similar fashion to a magnet


thermoratchet

The ratchet photocurrent includes the Seebeck thermoratchet effect as well as the effects of "linear" and "circular" ratchets, sensitive to the corresponding polarization of the driving electromagnetic force.

2015, P. Olbrich, J. Kamann, M. König, J. Munzert, L. Tutsch, J. Eroms, D.Weiss, Ming-Hao Liu, L.E. Golub, E.L. Ivchenko, V.V.Popov, D.V. Fateev, K.V. Mashinsky, F. Fromm, Th. Seyller, S.D. Ganichev, “Terahertz ratchet effects in graphene with a lateral superlattice”, in arXiv:

(physics) A device or system that changes temperature in one direction only


heliconical

The heliconical tilt angle, estimated from the orientational distribution functions (ODFs), in all cases increases from zero at the N - Ntb transition to approximately 27{\deg} at about 40 K below the transition, in excellent agreement with freeze fracture transmission electron microscopy results of Chen and the birefringence results of Meyer.

2015, Gautam Singh, Dena M. Agra-Kooijman, Michael R. Fisch, M. R. Vengatesan, Jang-Kun Song, Satyendra Kumar, “Orientational Order in the Nematic and Heliconical Nematic Liquid Crystals”, in arXiv:


rho meson

(physics) A short-lived hadronic isospin triplet.


technirho

We also present updated analyses of the walking technrho's for the diboson excesses by fully incorporating the constraints from the conformal barrier and the HLS as well as possible higher order effects: still characteristic of the one-family walking technirho is its smallness of the decay width, roughly of order #92;Gamma#47;M#95;#92;rho#92;sim#91;3#47;N#95;C#92;times 1#47;N#95;D#93;#92;times#91;#92;Gamma#47;M#95;#92;rho#93;#95;#123;#92;rmQCD#125;#92;,#92;simeq 70#92;,#123;#92;rmGeV#125;#47;2#92;,#123;#92;rmTeV#125; (N#95;D#61;N#95;C#61;4), in perfect agreement with the expected diboson resonance with #92;Gammalt;100#92;,#123;#92;rmGeV#125;.

2015, Hidenori S. Fukano, Shinya Matsuzaki, Koji Terashi, Koichi Yamawaki, “Conformal Barrier and Hidden Local Symmetry Constraints: Walking Technirhos in LHC Diboson Channels”, in arXiv:


電位

/ti̯ɛn⁵¹⁻⁵³ weɪ̯⁵¹/

/tiːn²² wɐi̯²²⁻³⁵/

/tiɛn²²⁻²¹ ui²²/

/tiɛn⁴¹⁻²² ui⁴¹/

/tiɛn²²⁻²¹ ui²²/

/tiɛn³³⁻¹¹ ui³³/

/tiɛn³³⁻²¹ ui³³/

/ti̯ɛn⁵¹⁻⁵³ weɪ̯⁵¹/

/tiːn²² wɐi̯²²⁻³⁵/

/tiɛn²²⁻²¹ ui²²/

/tiɛn⁴¹⁻²² ui⁴¹/

/tiɛn²²⁻²¹ ui²²/

/tiɛn³³⁻¹¹ ui³³/

/tiɛn³³⁻²¹ ui³³/


transresistivity

transresistivity (countable and uncountable, plural transresistivities)

The spin transresistivity coefficient is essentially enhanced in the diffusive regime, as compared to conventional predictions.

2015, A. G. Yashenkin, I. V. Gornyi, “Low-temperature spin Coulomb drag in a two-dimensional electron gas”, in arXiv:

(physics) resistivity to transport of electrons or other particles


SPLEED

spin-polarized low-energy electron diffraction#English

(uncountable, physics) Abbreviation of spin-polarized low-energy electron diffraction.


αιώρηση

head

αιώρηση • (aiórisi) n (plural αιωρήσεις)

aiórisi (romanization)
αιωρήσεις (plural)
αιώρηση (nominative singular)
αιωρήσεις (nominative plural)
αιώρησης (genitive singular)
αιωρήσεων (genitive plural)
αιώρηση (accusative singular)
αιωρήσεις (accusative plural)
αιώρηση (singular vocative)
αιωρήσεις (plural vocative)

el-decl-noun

Older or formal genitive singular: αιωρήσεως (aioríseos)


απλή αρμονική ταλάντωση

head

απλής αρμονικής ταλάντωσης

απλή αρμονική ταλάντωση • (aplí armonikí talántosi) f (plural απλής αρμονικής ταλάντωσης)

el-noun

απλής αρμονικής ταλάντωσης

aplí armonikí talántosi (romanization)
απλής αρμονικής ταλάντωσης (plural)

simple harmonic motion
simple harmonic motion

en-απλή_αρμονική_ταλάντωση-el-noun-WxvgP~RH


ταλάντωση

head

ταλάντωση • (talántosi) f (plural ταλαντώσεις)

talántosi (romanization)
ταλαντώσεις (plural)
ταλάντωση (nominative singular)
ταλαντώσεις (nominative plural)
ταλάντωσης (genitive singular)
ταλαντώσεων (genitive plural)
ταλάντωση (accusative singular)
ταλαντώσεις (accusative plural)
ταλάντωση (singular vocative)
ταλαντώσεις (plural vocative)

el-decl-noun

Older or formal genitive singular: ταλαντώσεως (talantóseos)

απλή αρμονική ταλάντωση


紅移

/hʊŋ²¹ jiː²¹/

/hʊŋ²¹ jiː²¹/


相對濕度

ㄒㄧㄤ ㄉㄨㄟˋ ㄕ ㄉㄨˋ

/ɕi̯ɑŋ⁵⁵ tu̯eɪ̯⁵¹ ʂʐ̩⁵⁵ tu⁵¹/

/sœːŋ⁵⁵ tɵy̯³³ sɐp̚⁵ tou̯²²/

/ɕi̯ɑŋ⁵⁵ tu̯eɪ̯⁵¹ ʂʐ̩⁵⁵ tu⁵¹/

/sœːŋ⁵⁵ tɵy̯³³ sɐp̚⁵ tou̯²²/


anentropy

en-noun

anentropy (countable and uncountable, plural anentropies)

Treivus has pointed out that the anentropy, apart from a constant factor (the universal gas constant) is equal to the chemical affinity for one componenent in a themodynamic system.

2001, Automatic Documentation and Mathematical Linguistics, page 15:

(physical chemistry, thermodynamics, countable and uncountable) A measure of the purity or chemical affinity in a thermodynamic system.


downlead

(electricity) An electrical cable connecting an outdoor structure to an indoor or in-ground structure.


○ and ◌⃝ for uses of a letter inside a circle


anticonfined

We show through several concrete examples that the behaviour of anticonfined singularities is strongly related to the integrability properties of such discrete mappings..

2015, Takafumi Mase, Ralph Willox, Alfred Ramani, Basil Grammaticos, “Integrable mappings and the notion of anticonfinement”, in arXiv:

(physics, of a singularity) Having an indefinite number of singular values


anticonfinement

We examine the notion of anticonfinement in the context of the singularity analysis of discrete systems.

(physics) The state of being anticonfined


azimuthon

We demonstrate that an incoherent ring-shaped optical pump creating the exciton-polariton confinement supports the existence of stationary and rotating azimuthon steady states with azimuthally modulated density.

2015, Guangyao Li, “Azimuthons and pattern formation in annularly confined exciton-polariton Bose-Einstein condensates”, in arXiv:

(physics) An exciton-polariton confined steady state with azimuthally modulated density


microcomb

This technique provides new degrees of freedom and enhanced flexibility in engineering the dispersion of microcomb resonators..

2015, Hojoong Jung, Menno Poot, Hong X. Tang, “In-resonator variation of waveguide cross-sections for dispersion control of aluminum nitride micro-rings”, in arXiv:

(physics) A microscopic comb used as a refraction grating


microstretch

We investigate linear theories of incompatible micromorphic elasticity, incompatible microstretch elasticity, incompatible micropolar elasticity and the incompatible dilatation theory of elasticity (elasticity with voids).

3853-3870 (2007), Markus Lazar, Gerard A. Maugin, “On microcontinuum field theories: the Eshelby stress tensor and incompatibility conditions”, in Philosophical Magazine, volumes 3853-3870, pages 3853–3870:

(physics) microscopic stretch (of a microelement of a solid)


microstretch

en-verb

microstretch (third-person singular simple present microstretches, present participle microstretching, simple past and past participle microstretched)

microstretches (present singular third-person)
microstretching (participle present)
microstretched (participle past)
microstretched (past)

(physics, transitive) To stretch microscopically.


offshell

Working at next-to-leading order in QCD we show that carefully selected ratios of offshell regions to onshell regions in the reconstructed top and antitop invariant mass spectra are, \emph{independently} of the coupling g#95;#123;tbW#125;, sensitive to the top-quark width.

2015, Stefan Liebler, Gudrid Moortgat-Pick, Andrew S. Papanastasiou, “Probing the top-quark width through ratios of resonance contributions of e⁺e⁻→W⁺W⁻b̄b”, in arXiv:

(mathematics, physics) That does not conform to classical physics.


bottomgate

(physics) A gate in contact with the bottom of a semiconductor


magnetodispersion

en-noun

magnetodispersion (countable and uncountable, plural magnetodispersions)

The weakly damped relativistic mode exhibits an unusual zigzag-shaped magnetodispersion dependence dictated by the diagonal component of the resistivity tensor #92;rho#95;#123;xx#125;.

2015, P.A. Gusikhin, V.M. Muravev, I.V. Kukushkin, “Dispersion of Volume Relativistic Magnetoplasma Excitation in a Gated Two-Dimensional Electron System”, in arXiv:

(physics) The dispersion of (or caused by) a magnetic field


ambitwistor

We obtain all the type II supergravity constraints in the pure spinor ambitwistor string by imposing consistency of local worldsheet gauge symmetries..

2015, Osvaldo Chandia, Brenno Carlini Vallilo, “On-shell type II supergravity from the ambitwistor pure spinor string”, in arXiv:

(mathematics, physics) A form of complex null geodesic


gravidynamics

We discuss the region of applicability of gravidynamics and its possible predictions for explanation of the modern observational and experimental data..

2015, A.B. Arbuzov, A.Yu. Cherny, D.J. Cirilo-Lombardo, R.G. Nazmitdinov, Nguyen Suan Han, A.E. Pavlov, V.N. Pervushin, A.F. Zakharov, “Von Neumann's Quantization of General Relativity”, in arXiv:


quadpolaron

An unexpected overweighted antipolaron is revealed in the quadpolaron state, and a hidden scaling behavior relevant to symmetry breaking is found in the bipolaron state.

2015, Zu-Jian Ying, Maoxin Liu, Hong-Gang Luo, Hai-Qing Lin, J. Q. You, “Ground-state phase diagram of the quantum Rabi model”, in arXiv:

(physics) A quasiparticle composed of two bipolarons


quasispin

The duality relations between the unitary and quasispin algebraic structures for the boson and fermion systems are extended to mixed boson-fermion system.

2015, M. A. Jafarizadeh, M. Ghapanvariy, N. Fouladiz, “Solvababe supersymmetric algebraic model for descriptions of transitional even and odd mass nuclei near the critical point of the spherical to unstable shapes”, in arXiv:

(physics) A quantum angular momentum associated with subatomic particles that exhibit collective behavior.


reggeized

The resummed collinear terms in transverse momentum space were calculated in Ref. [1] and correspond to the addition to the NLO BFKL kernel of a Bessel function of the first kind whose argument contains the strong coupling and a double logarithm of the ratio of the squared transverse momenta of the reggeized gluons.

2015, G. Chachamis, A. Sabio Vera, “A Monte Carlo study of double logarithms in the small x region”, in arXiv:


semitauonic

In particular semitauonic B decays can give important constraints on the charged Higgs sector.

1998, M. Rozanska, “On a feasibility of measuring exclusive semitauonic B0 decays at B-factories”, in Acta Physica Polonica, volume 29, numbers 7-8, page 2067:

Recent experimental results from the LHCb, BaBar and Belle collaborations on the semitauonic decays of B meson, #92;bar#123;B#125;#92;rightarrowD#123;(#92;ast)#125;#92;tau#92;bar#123;#92;nu#125;, showing a significant deviation from the Standard Model (SM), hint towards a new physics scenario beyond the SM.

2015, Chandan Hati, Girish Kumar, Namit Mahajan, “̄B→D^((∗))τ̄v excesses in ALRSM constrained from B, D decays and D⁰-̄D⁰ mixing”, in arXiv:


hypervirtual

(physics) Pertaining to spin orbitals of the complementary subspace (orthogonal to all closed-shell orbitals and all virtual orbitals).


magnomechanics

Our work demonstrates the fundamental principle of cavity magnomechanics and its application as a new information transduction platform based on coherent coupling between photons, phonons and magnons..

2015, Xufeng Zhang, Chang-Ling Zou, Liang Jiang, Hong X. Tang, “Cavity magnomechanics”, in arXiv:


asúigh

head

asúigh (present analytic asúnn, future analytic asúfaidh, verbal noun asú, past participle asúite)

asúnn (analytic present)
asúfaidh (analytic future)
asú (noun-from-verb)
asúite (participle past)
asúim (first-person indicative present singular)
asúnn tú (indicative present second-person singular)
asúir (indicative present second-person singular)
asúnn sé (indicative present singular third-person)
sí (indicative present singular third-person)
asúimid (first-person indicative plural present)
asúnn sibh (indicative plural present second-person)
asúnn siad (indicative plural present third-person)
asúid (indicative plural present third-person)
a asúnn (indicative present relative)
a asús (indicative present relative)
a n-asúnn (indicative present relative)
asúitear (autonomous indicative present)
d'asúigh mé (first-person indicative past singular)
d'asús (first-person indicative past singular)
asúigh mé‡ (first-person indicative past singular)
asús‡ (first-person indicative past singular)
d'asúigh tú (indicative past second-person singular)
d'asúis (indicative past second-person singular)
asúigh tú‡ (indicative past second-person singular)
asúis‡ (indicative past second-person singular)
d'asúigh sé (indicative past singular third-person)
sí (indicative past singular third-person)
asúigh sé (indicative past singular third-person)
sí‡ (indicative past singular third-person)
d'asúmar (first-person indicative past plural)
d'asúigh muid (first-person indicative past plural)
asúmar‡ (first-person indicative past plural)
asúigh muid‡ (first-person indicative past plural)
d'asúigh sibh (indicative past plural second-person)
d'asúbhair (indicative past plural second-person)
asúigh sibh‡ (indicative past plural second-person)
asúbhair‡ (indicative past plural second-person)
d'asúigh siad (indicative past plural third-person)
d'asúdar (indicative past plural third-person)
asúigh siad‡ (indicative past plural third-person)
asúdar‡ (indicative past plural third-person)
a d'asúigh (indicative past relative)
ar asúigh (indicative past relative)
asúdh (autonomous indicative past)
hasúdh (autonomous indicative past)
d'asúinn (first-person habitual indicative past singular)
asúinn‡ (first-person habitual indicative past singular)
n-asúinn‡‡ (first-person habitual indicative past singular)
d'asúiteá (habitual indicative past second-person singular)
asúiteá‡ (habitual indicative past second-person singular)
n-asúiteá‡‡ (habitual indicative past second-person singular)
d'asúdh sé (habitual indicative past singular third-person)
sí (habitual indicative past singular third-person)
asúdh sé (habitual indicative past singular third-person)
sí‡ (habitual indicative past singular third-person)
n-asúdh sé (habitual indicative past singular third-person)
sí‡‡ (habitual indicative past singular third-person)
d'asúimis (first-person habitual indicative past plural)
d'asúdh muid (first-person habitual indicative past plural)
asúimis (first-person habitual indicative past plural)
asúdh muid‡ (first-person habitual indicative past plural)
n-asúimis‡‡ (first-person habitual indicative past plural)
n-asúdh muid‡‡ (first-person habitual indicative past plural)
d'asúdh sibh (habitual indicative past plural second-person)
asúdh sibh‡ (habitual indicative past plural second-person)
n-asúdh sibh‡‡ (habitual indicative past plural second-person)
d'asúidís (habitual indicative past plural third-person)
d'asúdh siad (habitual indicative past plural third-person)
asúidís (habitual indicative past plural third-person)
asúdh siad‡ (habitual indicative past plural third-person)
n-asúidís‡‡ (habitual indicative past plural third-person)
n-asúdh siad‡‡ (habitual indicative past plural third-person)
a d'asúdh (habitual indicative past relative)
a n-asúdh (habitual indicative past relative)
d'asúití (autonomous habitual indicative past)
asúití‡ (autonomous habitual indicative past)
n-asúití‡‡ (autonomous habitual indicative past)
asúfaidh mé (first-person future singular)
asúfad (first-person future singular)
asúfaidh tú (future second-person singular)
asúfair (future second-person singular)
asúfaidh sé (future singular third-person)
sí (future singular third-person)
asúfaimid (first-person future plural)
asúfaidh muid (first-person future plural)
asúfaidh sibh (future plural second-person)
asúfaidh siad (future plural third-person)
asúfaid (future plural third-person)
a asúfaidh (future relative)
a asúfas (future relative)
a n-asúfaidh (future relative)
asúfar (autonomous future)
d'asúfainn (conditional first-person singular)
asúfainn‡ (conditional first-person singular)
n-asúfainn‡‡ (conditional first-person singular)
d'asúfá (conditional second-person singular)
asúfá‡ (conditional second-person singular)
n-asúfá‡‡ (conditional second-person singular)
d'asúfadh sé (conditional singular third-person)
sí (conditional singular third-person)
asúfadh sé (conditional singular third-person)
sí‡ (conditional singular third-person)
n-asúfadh sé (conditional singular third-person)
sí‡‡ (conditional singular third-person)
d'asúfaimis (conditional first-person plural)
d'asúfadh muid (conditional first-person plural)
asúfaimis‡ (conditional first-person plural)
asúfadh muid‡ (conditional first-person plural)
n-asúfaimis‡‡ (conditional first-person plural)
n-asúfadh muid‡‡ (conditional first-person plural)
d'asúfadh sibh (conditional plural second-person)
asúfadh sibh‡ (conditional plural second-person)
n-asúfadh sibh‡‡ (conditional plural second-person)
d'asúfaidís (conditional plural third-person)
d'asúfadh siad (conditional plural third-person)
asúfaidís‡ (conditional plural third-person)
asúfadh siad‡ (conditional plural third-person)
n-asúfaidís‡‡ (conditional plural third-person)
n-asúfadh siad‡‡ (conditional plural third-person)
a d'asúfadh (conditional relative)
a n-asúfadh (conditional relative)
d'asúfaí (autonomous conditional)
asúfaí‡ (autonomous conditional)
n-asúfaí‡‡ (autonomous conditional)
go n-asú mé (first-person present singular subjunctive)
go n-asúd (first-person present singular subjunctive)
go n-asú tú (present second-person singular subjunctive)
go n-asúir (present second-person singular subjunctive)
go n-asú sé (present singular subjunctive third-person)
sí (present singular subjunctive third-person)
go n-asúimid (first-person plural present subjunctive)
go n-asú muid (first-person plural present subjunctive)
go n-asú sibh (plural present second-person subjunctive)
go n-asú siad (plural present subjunctive third-person)
go n-asúid (plural present subjunctive third-person)
go n-asúitear (autonomous present subjunctive)
dá n-asúinn (first-person past singular subjunctive)
dá n-asúiteá (past second-person singular subjunctive)
dá n-asúdh sé (past singular subjunctive third-person)
sí (past singular subjunctive third-person)
dá n-asúimis (first-person past plural subjunctive)
dá n-asúdh muid (first-person past plural subjunctive)
dá n-asúdh sibh (past plural second-person subjunctive)
dá n-asúidís (past plural subjunctive third-person)
dá n-asúdh siad (past plural subjunctive third-person)
dá n-asúití (autonomous past subjunctive)
asúim (first-person imperative singular)
asúigh (imperative second-person singular)
asúdh sé (imperative singular third-person)
sí (imperative singular third-person)
asúimis (first-person imperative plural)
asúigí (imperative plural second-person)
asúidh (imperative plural second-person)
asúidís (imperative plural third-person)
asúitear (autonomous imperative)
asú (noun-from-verb)
asúite (participle past)
asúigh
n-asúigh
hasúigh

From ath- + súigh. Calque of French adsorber.

(transitive, physical chemistry, physics) adsorb (to accumulate on a surface, by adsorption)


asúire

asúire m (genitive singular asúire, nominative plural asúirí)

asúire (genitive singular)
asúirí (nominative plural)
nominative (indefinite)
asúire (indefinite singular)
asúirí (indefinite plural)
vocative (indefinite)
a asúire (indefinite singular)
a asúirí (indefinite plural)
genitive (indefinite)
dative (indefinite)
nominative (definite)
an t-asúire (definite singular)
na hasúirí (definite plural)
genitive (definite)
an asúire (definite singular)
na n-asúirí (definite plural)
dative (definite)
leis an asúire (definite singular)
don asúire (definite singular)
leis na hasúirí (definite plural)
asúire
n-asúire
hasúire
t-asúire

From asúigh (“adsorb; aspirate”, transitive verb) + -aire (agent noun suffix).


elastoresistivity

en-noun

elastoresistivity (countable and uncountable, plural elastoresistivities)

Comparing direct transport and elastoresistivity measurements, we extract the intrinsic resistivity anisotropy of strain-free samples.

2015, M. A. Tanatar, A. E. Böhmer, E. I. Timmons, M. Schütt, G. Drachuck, V. Taufour, S. L. Bud'ko, P. C. Canfield, R. M. Fernandes, R. Prozorov, “Origin of the Resistivity Anisotropy in the Nematic Phase of FeSe”, in arXiv:

(physics) A change in electrical resistivity as a result of elastic deformation


superalfvenic

en-adj

superalfvenic (comparative more superalfvenic, superlative most superalfvenic)

more superalfvenic (comparative)
most superalfvenic (superlative)

From super- + Alfvenic.
Etymology tree
English super-
English Alfven
English -ic
English Alfvenic
English superalfvenic.

etymon

Fast radiation-driven winds and supernovae input their huge kinetic power into the interstellar medium in the form of highly supersonic and superalfvenic outflows.

2015, Andrei Bykov, “Nonthermal particles and photons in starburst regions and superbubbles”, in Astronomy and Astrophysics Review, volume 2014:

(physics) Having a velocity greater than that of an Alfvén wave


Alfvenic

From Alfven + -ic.
Etymology tree
English Alfven
English -ic
English Alfvenic


thermofluidic

In essence, the dominance of Stokesian mechanics in such thermofluidic systems is established in the present study.

2015, Savithiri S, Purbarun Dhar, Arvind Pattamatta, Sarit K. Das, “Particle fluid interactivity deteriorates buoyancy driven thermal transport in nanosuspensions : A multi component lattice Boltzmann approach”, in arXiv:

(physics) Relating to the flow of heated fluids


短路

/tu̯än²¹⁴⁻²¹ lu⁵¹/

/te⁵³⁻⁴⁴ lɔ²²/

/te⁵⁵⁴⁻²⁴ lɔ⁴¹/

/te⁵³⁻⁴⁴ lɔ²²/

/te⁵³⁻⁴⁴ lɔ³³/

/te⁴¹⁻⁴⁴ lɔ³³/

/to⁵²⁻³⁵ lou¹¹/

/tu̯än²¹⁴⁻²¹ lu⁵¹/

/te⁵³⁻⁴⁴ lɔ²²/

/te⁵⁵⁴⁻²⁴ lɔ⁴¹/

/te⁵³⁻⁴⁴ lɔ²²/

/te⁵³⁻⁴⁴ lɔ³³/

/te⁴¹⁻⁴⁴ lɔ³³/

/to⁵²⁻³⁵ lou¹¹/

(electronics) to short circuit; to undergo a short circuit


gravoturbulent

As opposed to gravoturbulent fragmentation theories, we consider the dense core growth and demonstrate that the power law core mass function emerges independently of the initial distribution of density fluctuations by mass.

2015, Andrei Klishin, Igor Chilingarian, “Explaining the stellar initial mass function with the theory of spatial networks”, in arXiv:

gravitational collapse
gravitational collapse

(physics, astronomy) Relating to turbulence during the gravitational collapse of a star


magnetothermodynamics

In addition to a fluctuation-induced six-fold anisotropy present in zero field, an external magnetic field induces a combination of two-, three-, and six-fold clock terms as a function of its orientation providing for a rich and controllable magnetothermodynamics.

2015, V. S. Maryasin, M. E. Zhitomirsky, R. Moessner, “Low-field behavior of an XY pyrochlore antiferromagnet: emergent clock anisotropies”, in arXiv:

(physics) thermodynamics in the presence of a magnetic field


agyrotropy

Finally, the analysis of agyrotropy shows the presence of a distinct double structure laying^([sic]) all over the lower side facing the higher magnetic field region.

2015, Emanuele Cazzola, Maria Elena Innocenti, Stefano Markidis, Martin V. Goldman, David L. Newman, Giovanni Lapenta, “On the electron dynamics during island coalescence in asymmetric magnetic reconnection”, in arXiv:

electromagnetic radiation
electromagnetic radiation

(physics) A broken cylindrical symmetry in the movement of electromagnetic radiation required for collisionless magnetic reconnection; a loss of gyrotropy.


isogravity

Pure power-law density profiles, #92;rho(r)#92;proptor#123;b-3#125;, are classified in connection with the following reference cases: (i) isodensity, b#61;3, #92;rho#61; const; (ii) isogravity, b#61;2, g#61; const; (iii) isothermal, b#61;1, v#61;#91;GM(r)#47;r#93;#123;1#47;2#125;#61; const; (iv) isomass, b#61;0, M#61; const.

2015, R. Caimmi, “Gravitational acceleration and tidal effects in spherical-symmetric density profiles”, in arXiv:

electroweak interaction
electroweak interaction

(physics) A gauge theory that attempts to unify gravity with the electroweak interaction


isomass

If a packet of isomass ions is accelerated through the same potential difference, the ions will achieve an equal velocity and arrive at the detector with a time spread corresponding to their initial spatial distribution in the direction of the flight tube.

2004, Klaus G. Heumann, Handbook of Elemental Speciation: Techniques and Methodology, →ISBN:

In Fig. 4 the isomass lines of equal mₑₑ in the oscillation parameter space are shown, together with various bounds from existing and future reactor and accelerator oscillation experiments.

2010, H. V. Klapdor-Kleingrothaus, Seventy Years of Double Beta Decay, →ISBN:

Values of square root of area and mass/area of isomass lines for the Etna 1998 tephra deposit.

2013, Sarah A. Fagents, Tracy K. P. Gregg, Rosaly M. C. Lopes, Modeling Volcanic Processes: The Physics and Mathematics of Volcanism, →ISBN:

(physics) A condition of having the same mass.


isovorticed

In this paper we describe necessary and sufficient conditions on the vorticity function of a 2D ideal flow on a surface with or without boundary, for which there exists a steady flow among isovorticed fields.

2015, Anton Izosimov, Boris Khesin, “Characterization of steady solutions to the 2D Euler equation”, in arXiv:

(mathematics, physics) Having the same vorticity


photoabsorbance

en-noun

photoabsorbance (usually uncountable, plural photoabsorbances)

Results presented here demonstrate that fabrication of self organized nanostructures and development of oxygen vacancies, upon cobalt implantation, promote the enhancement of photoabsorbance in both UV (2 times) and visible (5 times) regimes.

2015, Shalik Ram Joshi, B. Padmanabhan, Anupama Chanda, Indrani Mishra, V. K. Malik, N. C. Mishra, D. Kanjilal, Shikha Varma, “Enhanced Photoabsorption from Cobalt Implanted Rutile TiO2 (110) Surfaces”, in arXiv:

(physics) The effect of (varying intensities of) light on the absorbance of a material


memresistance

In the high resistance state (HRS) the memresistance was in the order of MOhm leading to two independent selfsustained oscillators characterized by the different frequencies f1 and f2 and no phase relation between the oscillations.

2015, M. Ignatov, M. Hansen, M. Ziegler, H. Kohlstedt, “Synchronization of two memristive coupled van der Pol oscillators”, in arXiv:

(physics) Alternative form of memristance


neutronics

We used the Monte Carlo code MCNP5 to reproduce system neutronics in different operating conditions and to analyse neutron fluxes in the reactor core.

2015, Davide Chiesa, Massimiliano Clemenza, Stefano Pozzi, Ezio Previtali, Monica Sisti, Daniele Alloni, Giovanni Magrotti, Sergio Manera, Michele Prata, Andrea Salvini, Antonio Cammi, Matteo Zanetti, Alberto Sartori, “Fuel burnup analysis of the TRIGA Mark II Reactor at the University of Pavia”, in arXiv:

(physics) The flow of a stream of neutrons


axiodilaton

The former generate the standard flux superpotential for the axiodilaton and complex structure moduli.

2015, Adolfo Guarino, Gianluca Inverso, “Single-step de Sitter vacua from non-perturbative effects with matter”, in arXiv:

(physics) An axion and dilaton considered as a single particle


bogolon

The idea of this quasiparticle was introduced by Nikolay Bogolyubov in 1947, after whom it was named.

At low condensate density, the topology of the single-particle bands is transferred to the bogolon dispersion.

2015, O. Bleu, D.D. Solnyshkov, G. Malpuech, “Interacting quantum fluid in a polariton topological insulator”, in arXiv:

Bose-Einstein condensate
Bose-Einstein condensate

(physics) A collective excitation, in a Bose-Einstein condensate, that has some characteristics of a particle.


path loss

electromagnetic wave
electromagnetic wave

(physics) The attenuation of an electromagnetic wave as it propagates through space


leictreascóp

head

leictreascóp m (genitive singular leictreascóip, nominative plural leictreascóip)

leictreascóip (genitive singular)
leictreascóip (nominative plural)
nominative (indefinite)
leictreascóp (indefinite singular)
leictreascóip (indefinite plural)
vocative (indefinite)
a leictreascóip (indefinite singular)
a leictreascópa (indefinite plural)
genitive (indefinite)
leictreascóip (indefinite singular)
leictreascóp (indefinite plural)
dative (indefinite)
nominative (definite)
an leictreascóp (definite singular)
na leictreascóip (definite plural)
genitive (definite)
an leictreascóip (definite singular)
na leictreascóp (definite plural)
dative (definite)
leis an leictreascóp (definite singular)
don leictreascóp (definite singular)
leis na leictreascóip (definite plural)


虹吸

/xʊŋ³⁵ ɕi⁵⁵/

/hʊŋ²¹ kʰɐp̚⁵/

/xʊŋ³⁵ ɕi⁵⁵/

/hʊŋ²¹ kʰɐp̚⁵/


semiorthogonal

(physics) Orthogonal to the corresponding approximation space.


Vectorboson

de-noun

Vectorboson n (mixed, genitive Vectorbosons, plural Vectorbosonen)

Vectorbosons (genitive)
Vectorbosonen (plural)
Vectorboson (nominative singular)
Vectorbosonen (definite nominative plural)
Vectorbosons (genitive singular)
Vectorbosonen (definite genitive plural)
Vectorboson (dative singular)
Vectorbosonen (dative definite plural)
Vectorboson (accusative singular)
Vectorbosonen (accusative definite plural)


vibrodiffusion

Our results are: (i) the dimensionless advection equation contains \emph{two independent dimensionless small parameters}: the ratio of two time-scales and the spatial amplitudes of oscillations; (ii) we identify a sequence of \emph{distinguished limit solutions} which correspond to the successive degenerations of a \emph{drift velocity}; (iii) for a general oscillating velocity field we derive the averaged equations for the first \emph{four distinguished limit solutions}; (iv) we show, that \emph{each distinguish limit solution} produces an infinite number of \emph{parametric solutions} with a Strouhal number as the only large parameter; those solutions differ from each other by the slow time-scale and the velocity amplitude; (v) the striking outcome of our calculations is the inevitable appearance of \emph{vibrodiffusion}, which represents a Lie derivative of the averaged tensor of quadratic displacements; (vi) our main methodological result is the introduction of a logical order/classification of the solutions; we hope that it opens the gate for applications of the same ideas to more complex systems; (vii) five types of oscillating flows are presented as examples of different drifts and vibrodiffusion..

2015, Vladimir A Vladimirov, “Two-timing Hypothesis, Distinguished Limits, Drifts, and Vibrodiffusion for Oscillating Flows”, in arXiv:

(physics) diffusion by means of vibration


asqtad

The operators are constructed using HYP staggered quarks on the MILC asqtad lattice (N#95;f#61;2#43;1).

2015, Jangho Kim, Weonjong Lee, Jeonghwan Pak, Sungwoo Park, SWME Collaboration, “Nonperturbative Renormalization in the RI-SMOM Scheme and Gribov Uncertainty in the RI-MOM Scheme for Staggered Bilinears”, in PoS (LATTICE, volume 2015:

(physics) A staggered action arising when a gluon with momentum of order π/a is exchanged between quarks.


photogating

Furthermore, due to the strong photogating effect, these direct-band gap, multi-layer phototransistors produce ultra-high gains of (9.8 +- 2.5) x 10^4 A/W and inferred detectivities of (3.3 +- 0.8) x 10^13 Jones, putting In2Se3 amongst the most sensitive 2D materials for photodetection studied to date..

2015, Joshua O. Island, Sofya I. Blanter, Michele Buscema, Herre S.J. van der Zant, Andres Castellanos-Gomez, “Gate controlled photocurrent generation mechanisms in high-gain In2Se3 phototransistors”, in Nano Letters, volume 2015:


supermagnetosonic

From super- + magnetosonic or Blend of supersonic + magnetosonic.

The nonlinear evolution of the Kelvin Helmholtz instability in a magnetized plasma with a perpendicular flow close to, or in, the supermagnetosonic regime can produce a significant parallel-to-perpendicular pressure anisotropy.

2015, S. De Camillis, S. S. Cerri, F. Califano, F. Pegoraro, “Pressure anisotropy generation in a magnetized plasma configuration with a shear flow velocity”, in arXiv:


threetangle

I calculate the mixed threetangle #92;tau#95;3#91;#92;rho#93; for the reduced density matrices of the four-qubit representant states found in Phys.

2015, Andreas Osterloh, “The nine ways of four qubit entanglement and their threetangle”, in arXiv:

(physics) The entanglement of three qubits


campylon

We find that the flux depends only on a specific combination of campylon parameters, which we identify as the average campylon strength, and derive a universal flux law for the Poiseuille flow.

2015, J.-D. Debus, M. Mendoza, S. Succi, H. J. Herrmann, “Poiseuille flow in curved spaces”, in arXiv:

(physics) A localized metric perturbation in an intrinsicly curved medium.


attoclock

Tunneling time, formulated in various different forms due to the absence of a time operator in quantum theory, has been measured recently in experiments based on the attoclock in ultrafast laser ionization of Helium atoms [A.~Landsman {\it et al.}, Optica {\bf 1}, 343 (2014)].

2015, Durmus A. Demir, Tugrul Guner, “An Entropic Formulation of Tunneling Time”, in arXiv:

(physics) A device that can measure time intervals of the order of attoseconds


nanooptics

Potential of the analytical solutions for study of light fields in the various waveguides of nanooptics and nanoplasmonics are also discussed..

2015, N.M.Arslanov, Ali A.Kamli, S.A.Moiseev, “A transversely localized light in waveguide: the analytical solutions and its potential applications”, in arXiv:


diattenuation

Singular Mueller matrices play an important role in polarization algebra and have peculiar properties that stem from the fact that either the medium exhibits maximum diattenuation and/or polarizance, or because its associated canonical depolarizer has the property of fully randomizing, the circular component (at least) of the states of polarization of light incident on it.

2015, José J. Gil, Razvigor Ossikovski, Ignacio San José, “Singular Mueller matrices”, in arXiv:

(physics) attenuation of light that depends upon its polarization


photoferroelectrics

These results highlight the potential of the OMHP architecture for designing new functional photoferroelectrics and photopiezoelectrics..

2015, Shi Liu, Fan Zheng, Ilya Grinberg, Andrew M. Rappe, “Photoferroelectric and Photopiezoelectric Properties of Organometal Halide Perovskites”, in arXiv:

(physics) The study, design and manufacture of photoferroelectric devices


photopiezoelectrics

(physics) The study, design and manufacture of photopiezoelectric devices


photopiezoelectric

(physics) Of or relating to the effect of light on piezoelectric materials.


合力

/hɐp̚² lɪk̚²/

/hap̚¹²¹⁻²¹ liɪk̚¹²¹/

/hap̚⁴⁻³² liɪk̚⁴/

/hɐp̚² lɪk̚²/

/hap̚¹²¹⁻²¹ liɪk̚¹²¹/

/hap̚⁴⁻³² liɪk̚⁴/


單相

/tän⁵⁵ ɕi̯ɑŋ⁵¹/

/taːn⁵⁵ sœːŋ³³/

/tän⁵⁵ ɕi̯ɑŋ⁵¹/

/taːn⁵⁵ sœːŋ³³/

electrical engineering
electrical engineering

(electrical engineering) single-phasing; monophasic


頻譜

/pʰin³⁵ pʰu²¹⁴⁻²¹⁽⁴⁾/

/pʰin³⁵ pʰuɻʷ²¹⁴⁻²¹⁽⁴⁾/

/pʰɐn²¹ pʰou̯³⁵/

/pʰin³⁵ pʰu²¹⁴⁻²¹⁽⁴⁾/

/pʰin³⁵ pʰuɻʷ²¹⁴⁻²¹⁽⁴⁾/

/pʰɐn²¹ pʰou̯³⁵/


eptaplet

Of the two only viable candidates singled out in the original analysis, the scalar eptaplet has been found to decay too quickly to be around today, while the fermionic quintuplet will soon be probed by indirect Dark Matter (DM) searches.

2015, Eugenio Del Nobile, Marco Nardecchia, Paolo Panci, “Millicharge or Decay: A Critical Take on Minimal Dark Matter”, in arXiv:

(physics) A multiplet of seven related things


kilolambda

en-noun

kilolambda (plural kilolambdas or kilolambda)

kilolambdas (plural)
kilolambda (plural)

Archival ALMA observations at 820 micron on baselines up to 410 kilolambda are compared to parametrized disk models to determine the surface-brightness profile.

2015, Michiel R. Hogerheijde, David Bekkers, Paola Pinilla, Vachail N. Salinas, Mihkel Kama, Sean M. Andrews, Chunhua Qi, David J. Wilner, “Steepening of the 820 micron continuum surface-brightness profile signals dust evolution in TW Hya's disk”, in arXiv:


ppbar

Comparisons with ppbar and pp data reveal improvement in the description of single diffractive events..

2015, Christine O. Rasmussen, Torbjörn Sjöstrand, “Hard Diffraction with Dynamic Gap Survival”, in arXiv:

(physics) proton and antiproton (used attributively to describe a collision or other interaction of these two particles)


supercondensation

LL-Q1860 (eng)-Flame, not lame-supercondensation.wav

The macroscopic dipole develops around two equilibrium fixed points, demonstrating condensation in real space; the fixed points are located exactly, both near the transition, and in the supercondensation regime at large energies.

2015, Xiaoquan Yu, Thomas P. Billam, Jun Nian, Matthew T. Reeves, Ashton S. Bradley, “Vortex Clustering Transition in a Confined 2D Quantum Fluid”, in arXiv:

(physics) condensation to form a superfluid


eigenchannel

The calculation of the diffusion coefficient and the energy density profile of the most transmitted eigenchannel clearly exhibits the transition of transport behaviour from diffusion to localization..

2015, Yuchen Xu, Hao Zhang, Yujun Lin, Heyuan Zhu, “Light transport behaviours in quasi-1D disordered waveguides composed of random photonic lattices”, in arXiv:

(physics) The superposition of coupled physical channels with a common phase (the eigenphase).


magnetoelastics

Here, we combine this principle with elements of magnetoelastics, and show that optical excitation of pairs of infrared-active optical phonons can excite coherent spin waves in the rare-earth orthoferrite ErFeO#95;3.

2015, T. F. Nova, A. Cartella, A. Cantaluppi, M. Foerst, D. Bossini, R. V. Mikhaylovskiy, A. V. Kimel, R. Merlin, A. Cavalleri, “An effective magnetic field from optically driven phonons”, in arXiv:

(physics) The physics of magnetoelasticity


magnetothermopower

magnetothermopower (countable and uncountable, plural magnetothermopowers)

Furthermore, we obtain dramatic variations of both the magnetothermopower and the spin Seebeck effect, which suggest that in our device spin currents can be controlled with temperature gradients only..

2015, Sun-Yong Hwang, Rosa Lopez, David Sanchez, “Large thermoelectric power and figure of merit in a ferromagnetic-quantum dot-superconducting device”, in arXiv:


cosmokinematics

In this work we use cosmography to alleviate the degeneracy among cosmological models, proposing a way to parameterize matter and dark energy in terms of cosmokinematics quantities.

2015, Orlando Luongo, Giovanni Battista Pisani, Antonio Troisi, “Cosmological degeneracy versus cosmography: a cosmographic dark energy model”, in arXiv:

(physics, astronomy) The study of the motion or the universe


elastocapillarity

Within this framework, the composite stiffness depends solely on the ratio of the elastocapillarity length L to the inclusion radius R.

2015, Francesco Mancarella, Robert W. Style, John S. Wettlaufer, “Interfacial tension and a three-phase generalized self-consistent theory of non-dilute soft composite solids”, in arXiv:


optocapillary

Our device facilitates resonantly-enhanced optocapillary interactions that might enable optical excitation (/cooling) of capillary droplet-modes, including with the most-common and important liquid - water..

2015, Shai Maayani, Leopoldo L. Martin, Samuel Kaminski, Tal Carmon, “Cavity Optocapillaries”, in arXiv:

(physics) Relating to the interaction of light on capillary effects


photoconvective

The photoconvective forces demonstrated here provide a new tool for high bandwidth control of mechanical motion in cryogenic conditions, and have the potential to allow efficient transfer of electromagnetic energy to motional kinetic energy..

2015, D. L. McAuslan, G. I. Harris, C. Baker, Y. Sachkou, X. He, E. Sheridan, W. P. Bowen, “Microphotonic Forces From Superfluid Flow”, in arXiv:


photoconvection

(physics) convection under the influence of light


axizilla

The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10#123;-38#125;#92;,#92;textrm#123;cm#125;²..

2015, Jihn E. Kim, “Is an axizilla possible for di-photon resonance?”, in arXiv:

(physics) A heavy form of axion in an extension of the Standard Model


barristor

(physics) A form of solid-state triode that features a variable barrier


multiqudit

We discuss the hidden correlations in single-qudit states as a new resource for quantum technologies analogous to the known resource in correlations associated with the entanglement in multiqudit systems..

2015, Margarita A Man'ko, Vladimir I Man'ko, “Hidden correlations in indivisible qudits as a resource for quantum technologies on examples of superconducting circuits”, in arXiv:


nonbirefringence

This nonbirefringence constrains the spacetime constitutive tensor to high precision to a core metric form with an axion degree and a dilaton degree of freedom.

2015, Wei-Tou Ni, “Equivalence Principles, Spacetime Structure and the Cosmic Connection”, in arXiv:

(physics) The condition of being nonbirefringent


paramagnetoelectric

The value of the paramagnetoelectric (PME) coefficient shows a pronounced maximum near the ferroelectric-to-paraelectric phase transition temperature, T_C, and then decreases sharply to zero for T>T_C.

2015, V. V. Laguta, A. N. Morozovska, E. A. Eliseev, I. P. Raevski, S. I. Raevskaya, E. I. Sitalo, S. A. Prosandeev, L. Bellaiche, “Room-temperature paramagnetoelectric effect in magnetoelectric multiferroics Pb(Fe1/2Nb1/2)O3 and its solid solution with PbTiO3”, in arXiv:

(physics) Describing the effect of an electric field on paramagnetic materials


photogain

At a reverse bias of 3V, we achieve avalanche multiplication, with 0.37A/W responsivity and avalanche photogain~2.

2015, Ilya Goykhman, Ugo Sassi, Boris Desiatov, Noa Mazurski, Silvia Milana, Domenico de Fazio, Anna Eiden, Jacob Khurgin, Joseph Shappir, Uriel Levy, Andrea C. Ferrari, “On-chip integrated, silicon-graphene plasmonic Schottky photodetector, with high responsivity and avalanche photogain”, in arXiv:

(physics) The gain (multiplication factor) of a photodetector or photomultiplier


protostring

If the transverse space of the protostring could be "decompactified", string bit models might provide an appealing and solid foundation for superstring theory..

2015, Charles B. Thorn, “1/N Perturbations in Superstring Bit Models”, in arXiv:

(physics, string theory) A hypothetical precursor to a fundamental string that can evolve into a fundamental string as the higher dimensions compactify.


semigrand

A cluster algorithm for Monte Carlo simulations in a semigrand ensemble was used.

2015, Wojciech T. Góźdź, Alina Ciach, “Critical Point Calculation for Binary Mixtures of Symmetric Non-additive Hard Disks”, in arXiv:

(physics) Pertaining to a distribution of species that holds the number of particles, pressure, and temperature fixed but allows mole fractions of species within a phase to fluctuate.


superferromagnetic

In the superferromagnetic phase the magnetization response exhibited remarkable anisotropy, with anomalously large polar magnetization in the applied magnetic filed, which decreases approaching the film percolation transition.

2015, N. N. Kovaleva, A. A. Gorbatsevich, A. V. Bagdinov, O. Stupakov, E. I. Demikhov, A. Dejneka, F. A. Pudonin, “Unveiling superferromagnetic polar state in inhomogeneous nanoisland FeNi films featuring anomalously strong planar diamagnetic response near percolation transition”, in arXiv:

(physics) Relating to superferromagnetism


thermovoltage

This thermo-phase increases up to a maximal value of #92;pi#47;2 after which thermovoltage is expected to develop.

2015, Yaakov Kleeorin, Yigal Meir, Yonatan Dubi, “Large Tunable Thermophase in Superconductor -- Quantum Dot -- Superconductor Josephson Junctions”, in arXiv:


transrelativistic

Such choked jets may explain transrelativistic SNe and low-luminosity (LL) GRBs.

2015, Nicholas Senno, Kohta Murase, Peter Meszaros, “Choked Jets and Low-Luminosity Gamma-Ray Bursts as Hidden Neutrino Sources”, in arXiv:

(physics) Describing a transition from a nonrelativistic to a relativistic one


photogravitational

The case of the planar circular photogravitational restricted three-body problem where the more massive primary is an emitter of radiation is numerically investigated.

2015, Euaggelos E. Zotos, “Unveiling the influence of the radiation pressure in nature of orbits in the photogravitational restricted three-body problem”, in A&SS, volume 2015:

(physics, astronomy) Describing the effects of light radiation on the gravitational attraction to a star


sub-qubit

A solution for fault tolerant quantum computation with arbitrary length is concatenated coding, where each qubit is encoded by a block of n sub-qubits, each sub-qubit being encoded by other n blocks of qubits, and so on […].

2005, Mihai Udrescu-Milosav, Quantum Circuits Engineering: Efficient Simulation and Reconfigurable Quantum Hardware, Politehnica University of Timişoara, pages 74–75:

We present a trade-off relation satisfied by these maximal violations, which gives rise to restrictions on the distribution of nonlocality among the subqubit systems.

062339 (2015), Hui-Hui Qin, Shao-Ming Fei, Xianqing Li-Jost, “Trade-off Relations of Bell Violations among Pairwise Qubit Systems”, in Physical Review A, volume 062339:

(physics) A quantity of information less than one qubit, or a physical system used to represent such a quantity.


coorbit

As special cases, this includes embeddings into Sobolev spaces of (homogeneous and inhomogeneous) Besov spaces, (#92;alpha)-modulation spaces, shearlet smoothness spaces and also of a large class of wavelet coorbit spaces, in particular of shearlet-type coorbit spaces. Precisely, we will show that under extremely mild assumptions on the covering #92;mathcal#123;Q#125;#61;#92;left(Q#95;#123;i#125;#92;right)#95;#123;i#92;inI#125;, we have #92;mathcal#123;D#125;#92;left(#92;mathcal#123;Q#125;,L#123;p#125;,Y#92;right)#92;hookrightarrowW#123;k,q#125;(#92;mathbb#123;R#125;#123;d#125;) as soon as p#92;leqq and Y#92;hookrightarrow#92;ell#95;#123;u#123;#92;left(k,p,q#92;right)

2016, Felix Voigtlaender, “Embeddings of Decomposition Spaces into Sobolev and BV Spaces”, in arXiv:

(mathematics, physics) The dual of an orbit


echellette

We use the HST photometry from WFPC2 and WFC3 images obtained with UV and optical filters, as well as MagE echellette spectrograph data from the Las Campanas Clay 6.5m telescope, in order to construct the observed UV/optical SED of NGC 7252: W3.

2016, I. Cabrera-Ziri, N. Bastian, M. Hilker, B. Davies, F. Schweizer, J. M. D. Kruijssen, A. Mejía-Narváez, F. Niederhofer, T. D. Brandt, M. Rejkuba, G. Bruzual, G. Magris, “Is the Escape Velocity in Star Clusters Linked to Extended Star Formation Histories? Using NGC 7252: W3 as a Test Case”, in arXiv:


precompound

We explore the emission of light fragments through each of these mechanisms and demonstrate an improved agreement with experimental data achieved by extending precompound models to include emission of fragments heavier than ⁴He..

2016, Leslie M. Kerby, Stepan G. Mashnik, Konstantin K. Gudima, Arnold J. Sierk, Jeffrey S. Bull, Michael R. James, “Energetic Light Fragment Production Capability in MCNP6”, in arXiv:

(physics) Occurring just before the formation of an excited compound nucleus, when an incoming nucleon interacts with nucleons on the surface of the nucleus.


viscoelastoplastic

A PDE system consisting of the momentum balance, mass balance, and energy balance equations for displacement, capillary pressure, and temperature as a model for unsaturated fluid flow in a porous viscoelastoplastic solid is shown to admit a solution under appropriate assumptions on the constitutive behavior.

2016, Bettina Albers, Pavel Krejci, Elisabetta Rocca, “Solvability of an unsaturated porous media flow problem with thermomechanical interaction”, in arXiv:

(physics) Viscoelastic and plastic or viscous and elastoplastic.


cryptoquark

One can implement the "massless quark" solution in a phenomenologically acceptable way, by using a massless quark that is always confined within superheavy particles, and is therefore effectively superheavy: a cryptoquark.

2016, Frank Wilczek, “Superheavy Light Quarks and the Strong P, T Problem”, in arXiv:

(physics) A massless quark that is trapped by a superheavy particle.


degrate

en-verb

degrate (third-person singular simple present degrates, present participle degrating, simple past and past participle degrated)

degrates (present singular third-person)
degrating (participle present)
degrated (participle past)
degrated (past)

This work demonstrates the existence of distinct mechanisms that degrate the quantum electronic effects in graphene, which are affected differently by the sample production methodology..

2016, Fabio M. Ardito, Thiago G. Mendes-de-Sa, Paulo F. Gomes, Daniela L. Mafra, Rodrigo G. Lacerda, F. Iikawa, Eduardo Granado, “Landau Level Broadening Mechanisms of Neutral Graphene: Strain Fields versus Fermi Velocity Distribution”, in arXiv:

(physics) To remove the property of a grating from


hypoequilibrium

They are derived via the concepts of hypoequilibrium state and nonequilibrium intensive properties, which describe the nonmutual equilibrium status between subspaces of the thermodynamic state space of a single system and/or of the state space of the two interacting systems.

2016, Guanchen Li, Michael R. von Spakovsky, “Steepest-entropy-ascent quantum thermodynamic modeling of the far-from-equilibrium interactions between nonequilibrium systems of indistinguishable particle ensembles”, in arXiv:

(physics) A state that is in some way less than an equilibrium


supersymmetrize

supersymmetrize (third-person singular simple present supersymmetrizes, present participle supersymmetrizing, simple past and past participle supersymmetrized)

supersymmetrizes (present singular third-person)
supersymmetrizing (participle present)
supersymmetrized (participle past)
supersymmetrized (past)

(physics) To convert to a form compatible with supersymmetry


supervirial

LL-Q1860 (eng)-Flame, not lame-supervirial.wav

For example, the 0.5-2 Myr old Orion Nebula Cluster ( ONC ), which is known to be supervirial with a virial mass about twice the observed mass ( Hillenbrand & Hartmann 1998 ), has already expelled its residual gas and is expanding rapidly.

2008, Johan Hendrik Knapen, T. J. Mahoney, Alexandre Vazdekis, Pathways Through an Eclectic Universe, page 6:

For many of the young (~10Myr) star clusters M_(dyn) >> Mₚₕₒₜ Goodwin & Bastian (2006) suggest that this is a signature of gas expulsion and the 'infant mortality' scenario discussed in Section 2.1, i.e., they conclude that these clusters are supervirial.

2010, Mark Gieles, “Star Cluster Disruption”, in Richard de Grijs, Jacques R. D. Lépine, editors, Star Clusters (IAU S266): Basic Galactic Building Blocks, page 75:

If measured early enough (lt;2 Myr in our simulations, or #92;sim20 crossing times), the velocity dispersion can be used to determine whether a region was highly supervirial at birth without the risk of degeneracy.

2016, Richard J. Parker, Nicholas J. Wright, “Dynamical evolution of star forming regions - II. Basic kinematics”, in arXiv:

It is subvirial when Q < 1, which corresponds to a negative acceleration of the polar inertia moment, Ï < 0 (initial contraction) and supervirial when Q >1, which corresponds to a positive acceleration of the polar inertia moment, Ï > 0 (initial expansion).

2019, Roberto A. Capuzzo Dolcetta, Classical Newtonian Gravity:, page 57:

(physics) Expanding at an accelerating rate.


dark soliton

(physics) A localized surface soliton that causes a temporary decrease in an associated wave amplitude


bright soliton

(physics) A localized surface soliton that causes a temporary increase in an associated wave amplitude


antidark

This interaction involves the mutual collision between multi-peak solitons as well as the interplay of multi-peak soliton and other types of localized nonlinear waves (breather and antidark soliton).

2016, Liang Duan, Zhan-Ying Yang, Chong Liu, Wen-Li Yang, “Prolific interaction structures and shape-changing collisions in an erbium-doped fiber system”, in arXiv:

(physics) Describing a form of bright soliton


metamirror

In addition to offering a possibility to realize extremely small focal distances, metamirror antennas are practically penetrable and invisible for any radiation outside of the operating frequency range..

2016, Svetlana N. Tcvetkova, Viktar S. Asadchy, Sergei A. Tretyakov, “Scanning characteristics of metamirror antennas with sub-wavelength focal distance”, in arXiv:

(physics) A surface composed of single planar array of electrically small bianisotropic inclusions


hyperferroelectric

(physics) A ferroelectric (material) that has a spontaneous polarization


bunchlet

For the TS design assumed, the field of an incident bunchlet on the holes is not only coupled to the output but is also scattered back into the beam pipe, exciting waves in both directions.

1993, J Rossbach, High Energy Accelerators, page 892:

In the CLIC design the drive linac uses four trains spaced by 2.84 ns of 43 bunchlets (1 cm bunchlet spacing, 40 nC each) to produce via the transfer structures 30 GHz power pulses of 40 MW for the main linac.

1994, G. Carron, L. Thorndahl, “Progress with the CLIC Transfer Structures (CTS)”, in Christine Petit-jean-genaz, Vic Suller, editors, European Particle Accelerator Conference (Epac 94):

This drive-linac conceptual design implies certain challenges which have been addressed, mainly the bunchlet generation, the transfer structure design and the beam dynamics control.

2014, M. Dienes, M. Month, B. Strasser, Frontiers of Particle Beams: Factories with e+ e- Rings, page 165:

particle accelerator
particle accelerator

(physics) A very short burst of subatomic particles in the beam of a particle accelerator.


gasdynamic

The Lagrangian, multi-dimensional, ideal, compressible gasdynamic equations are written in a multi-symplectic form, in which the Lagrangian fluid labels, mⁱ (the Lagrangian mass coordinates) and time t are the independent variables, and in which the Eulerian position of the fluid element #123;#92;bfx#125;#61;#123;#92;bfx#125;(#123;#92;bfm#125;,t) and the entropy S#61;S(#123;#92;bfm#125;,t) are the dependent variables.

2016, G. M. Webb, S.C. Anco, “Vorticity and Symplecticity in Multi-Symplectic Lagrangian Gas Dynamics”, in Journal of Physics A, volumes Mathematical and Theoretical:


magnetovolume

The coexistence of spin-states and observation of history-depending irreversibility is explained as effect of long-range elastic strains mediated by magnetovolume coupling.

2016, N. Martin, I. Mirebeau, M. Deutsch, J.-P. Itié, J.-P. Rueff, U.K. Rössler, K. Koepernik, L.N. Fomicheva, A.V. Tsvyashchenko, “Magnetovolume effect, macroscopic hysteresis and moment collapse in the paramagnetic state of cubic MnGe under pressure”, in arXiv:

(physics) Relating to the change of volume of a crystal lattice in a magnetic field


multipolaron

In this article, we investigate the asymptotic behavior of the ground state energy of the Fr\"ohlich Hamiltonian for a Fermionic multipolaron in the so-called strong coupling limit.

2016, Ioannis Anapolitanos, Michael Hott, “Asymptotic behavior of the ground state energy of a Fermionic Fröhlich multipolaron in the strong coupling limit”, in arXiv:

(physics) A quasiparticle composed of multiple polarons


counterdiabatic

Here we present the first experimental realization of counterdiabatic driving in a continuous variable system, implementing a shortcut to the adiabatic transport of a trapped ion, in which nonadiabatic transitions are suppressed during all stages of the process.

2016, Shuoming An, Dingshun Lv, Adolfo del Campo, Kihwan Kim, “Shortcuts to Adiabaticity by Counterdiabatic Driving in Trapped-ion Transport”, in arXiv:


supercollimation

In photonic crystals, such thresholdless #92;mathcal#123;PT#125; transitions are shown to yield significant control over the band structure of the system, and can result in all-angle supercollimation, a #92;mathcal#123;PT#125;-superprism effect, and unidirectional behavior..

2016, Alexander Cerjan, Aaswath Raman, Shanhui Fan, “Exceptional contours and band structure design in parity-time symmetric photonic crystals”, in arXiv:

(physics) The focusing of radiation into a finite-width beam that shows very little diffraction.


聲速

/ʂɤŋ⁵⁵ su⁵¹/

/sɪŋ⁵⁵ t͡sʰʊk̚⁵/

/siɪŋ³³ sɔk̚⁵/

/siɪŋ⁴⁴⁻²² sɔk̚³²/

/ʂɤŋ⁵⁵ su⁵¹/

/sɪŋ⁵⁵ t͡sʰʊk̚⁵/

/siɪŋ³³ sɔk̚⁵/

/siɪŋ⁴⁴⁻²² sɔk̚³²/


subclosure

However the first excited state (0#95;2#43;) has #123;12#125;C#43;alpha cluster structure and this state is largely affected by the increase of the strength; the subclosure configuration of the p#95;#123;3#47;2#125; shell for the #123;12#125;C cluster part becomes more important than three alpha configuration.

2016, H. Matsuno, N. Itagaki, “Effect of cluster-shell competition of ¹²C on E0 transitions in ¹⁶O”, in arXiv:


駐波

/ʈ͡ʂu⁵¹ pu̯ɔ⁵⁵/

/t͡syː³³ pɔː⁵⁵/

/ʈ͡ʂu⁵¹ pu̯ɔ⁵⁵/

/t͡syː³³ pɔː⁵⁵/

(physics) standing wave; stationary wave


靜力學

ㄐㄧㄥˋ ㄌㄧˋ ㄒㄩㄝˊ

/t͡ɕiŋ⁵¹⁻⁵³ li⁵¹ ɕy̯ɛ³⁵/

/t͡sɪŋ²² lɪk̚² hɔːk̚²/

/t͡ɕiŋ⁵¹⁻⁵³ li⁵¹ ɕy̯ɛ³⁵/

/t͡sɪŋ²² lɪk̚² hɔːk̚²/


超對稱

/ʈ͡ʂʰɑʊ̯⁵⁵ tu̯eɪ̯⁵¹⁻⁵³ ʈ͡ʂʰən⁵¹/

/ʈ͡ʂʰɑʊ̯⁵⁵ tu̯eɪ̯⁵¹⁻⁵³ ʈ͡ʂʰɤŋ⁵¹/

/t͡sʰiːu̯⁵⁵ tɵy̯³³ t͡sʰɪŋ³³/

/ʈ͡ʂʰɑʊ̯⁵⁵ tu̯eɪ̯⁵¹⁻⁵³ ʈ͡ʂʰən⁵¹/

/ʈ͡ʂʰɑʊ̯⁵⁵ tu̯eɪ̯⁵¹⁻⁵³ ʈ͡ʂʰɤŋ⁵¹/

/t͡sʰiːu̯⁵⁵ tɵy̯³³ t͡sʰɪŋ³³/


同步加速器

ㄊㄨㄥˊ ㄅㄨˋ ㄐㄧㄚ ㄙㄨˋ ㄑㄧˋ

тунбу цзясуци

/tʰʊŋ³⁵ pu⁵¹ t͡ɕi̯ä⁵⁵ su⁵¹⁻⁵³ t͡ɕʰi⁵¹/

/tʰʊŋ²¹ pou̯²² kaː⁵⁵ t͡sʰʊk̚⁵ hei̯³³/

/tʰʊŋ³⁵ pu⁵¹ t͡ɕi̯ä⁵⁵ su⁵¹⁻⁵³ t͡ɕʰi⁵¹/

/tʰʊŋ²¹ pou̯²² kaː⁵⁵ t͡sʰʊk̚⁵ hei̯³³/


Darwin drift

Named after Sir Charles Galton Darwin, who proved a related theorem in 1953.

z-component of any force on the surface of the swimmer and ρ the radial co- ordinate. v D is termed the Darwin drift: by comparison, for a colloid at zero Reynolds number this quantity is infinite. The magnitude of the Darwin drift is of the order.

2016, C.N. Likos, F. Sciortino, E. Zaccarelli, Soft Matter Self-Assembly, →ISBN, page 392:

(fluid dynamics) The phenomenon by which a fluid parcel is permanently displaced after the passage of a body through a fluid – the fluid being at rest far away from the body.


Dickenrücklage

de-noun

Dickenrücklage f (genitive Dickenrücklage, plural Dickenrücklagen)

Dickenrücklage (genitive)
Dickenrücklagen (plural)
Dickenrücklage (nominative singular)
Dickenrücklagen (definite nominative plural)
Dickenrücklage (genitive singular)
Dickenrücklagen (definite genitive plural)
Dickenrücklage (dative singular)
Dickenrücklagen (dative definite plural)
Dickenrücklage (accusative singular)
Dickenrücklagen (accusative definite plural)

/ˈdɪkənˈʁʏkˌlaːɡə/

(aerodynamics) location of maximum thickness (in an airfoil, the distance between the leading edge and the chord point of maximum thickness)


multichimera

The multichimera state is shown to have a power law distribution of synchronized cluster sizes, whose exponent is found to be independent of the system parameters..

2016, Amitava Banerjee, Muktish Acharyya, “Synchronized, Chimera and Multichimera States in Simple Cellular Automata Model of Coupled Oscillators”, in arXiv:

(physics) A complex spatiotemporal pattern consisting of multiple coexisting domains of synchronized dynamics within a domain of incoherent dynamics, produced by a system of nonlocally coupled oscillators.


vinkelhastighed

vinkelhastighed (indefinite nominative singular)
vinkelhastigheden (definite nominative singular)
vinkelhastigheder (indefinite nominative plural)
vinkelhastighederne (definite nominative plural)
vinkelhastigheds (genitive indefinite singular)
vinkelhastighedens (definite genitive singular)
vinkelhastigheders (genitive indefinite plural)
vinkelhastighedernes (definite genitive plural)


asymmetron

From the neuter substantive form of Ancient Greek ἀσύμμετρος (asúmmetros, “asymmetrical”).

der

Our model is formally similar to the asymmetron scenario recently introduced in application to cosmology, though here we are interested in consequences for neutron stars and thus consider a mass term that does not modify the geometry on cosmological scales.

2016, Fethi M. Ramazanoğlu, Frans Pretorius, “Spontaneous Scalarization with Massive Fields”, in arXiv:

(physics) A massive scalar field proposed as a form of dark matter


monoparticular

We also show that the new proposal for the partition function does not produce any inconsistency for a system of distinguishable localized particles, where the monoparticular partition function is not extensive..

2016, A. Fernandez-Peralta, Raul Toral, “Ensemble equivalence for distinguishable particles”, in arXiv:


parastatistic

The parastatistic distribution of a total debt owed to a large number of creditors is considered in relation to the duration of these debts.

2016, I.A. Molotkov, N.A. Ryabova, “Critical value of the total debt in view of the debts durations”, in arXiv:


supermodulation

LL-Q1860 (eng)-Flame, not lame-supermodulation.wav

This supermodulation has a periodicity nearly commensurate with four lattice constants in-plane, eight out-of-plane, with long correlation lengths in three dimensions.

2016, Junfeng He, Padraic Shafer, Thomas R. Mion, Vu Thanh Tra, Qing He, J. Kong, Y.-D. Chuang, W. L. Yang, M. J. Graf, J.-Y. Lin, Y.-H. Chu, E. Arenholz, Rui-Hua He, “Observation of a Three-Dimensional Quasi-Long-Range Electronic Supermodulation in YBa2Cu3O7-x/La0.7Ca0.3MnO3 Heterostructures”, in arXiv:

(physics) modulation of a material's superconductivity


superpenalization

LL-Q1860 (eng)-Flame, not lame-superpenalization.wav

And we prove the optimal order of convergence in energy norm and L²-norm by the superpenalization technique.

2016, Zhihao Ge, Xiaogang Zhu, “Analysis of new stabilized hp discontinuous Galerkin methods for elasticity problem”, in arXiv:


multicaloric

The resulting equations for electrically and magnetically induced multicaloric effects are incorrect and cannot be used for measurement interpretation..

2016, Ivan A. Starkov, Alexander S. Starkov, “Rebuttal of "The multicaloric effect in multiferroic materials"”, in arXiv:

(physics) Both magnetocaloric and electrocaloric


permuton

Introduced by Carlos Hoppen, Yoshiharu Kohayakawa, Carlos Gustavo Moreira, Balázs Ráth and Rudini Menezes Sampaio in their 2011 paper, "Limits of permutation sequences", with the name "limit permutation".
The term "permuton" was coined by Roman Glebov, Andrzej Grzesik, Tereza Klimošová and Daniel Kráľ in their 2013 paper, "Finitely forcible graphons and permutons", from permute, to resemble graphon.

In the recent terminology of permutons, our work can be interpreted as the convergence of uniform random separable permutations towards a "Brownian separable permuton"..

2016, Frédérique Bassino, Mathilde Bouvel, Valentin Féray, Lucas Gerin, Adeline Pierrot, “The Brownian limit of separable permutations”, in arXiv:

(mathematics, physics) A probability measure Φ on the σ-algebra of Borel sets of the unit square [0,1]² such that Φ has uniform marginals (that is, Φ ([α, β] × [0,1]) = Φ ([0,1] × [α, β]) = β − α for every 0 ≤ α ≤ β ≤ 1).


selfconjugate

Interestingly, some of the solutions are not selfconjugate, which puts the model in sharp contrast to one of the model's limiting cases, the Heisenberg xxx spin chain.

2016, Rob Klabbers, “Thermodynamics of Inozemtsev's Elliptic Spin Chain”, in arXiv:

(mathematics, physics) Alternative form of self-conjugate


hyperquantum

Finally, we determine the dominant term of the R\'enyi entropies of the Rydberg states explicitly in terms of the hyperquantum numbers (n,l), the parameter order p and the universe dimensionality D for all possible cases D#92;ge 1.

2016, A.I. Aptekarev, D.N. Tulyakov, I.V. Toranzo, J.S. Dehesa, “Rényi entropies of the highly-excited states of multidimensional harmonic oscillators by use of strong Laguerre asymptotics”, in arXiv:

(physics) Pertaining to values at which a quantum-mechanical equation approaches infinity.


ακινησία

akinisía (romanization)
ακινησία (nominative singular)
ακινησίας (genitive singular)
ακινησία (accusative singular)
ακινησία (singular vocative)


torsiton

(physics) A quantum of torsional electronic vibration


electroconvective

When the buoyancy destabilizes the flow, it alters the electroconvective patterns by introducing upward and downward fingers of respectively light and heavy fluid..

2016, Elif Karatay, Matthias Wessling, Ali Mani, “On the coupling between buoyancy forces and electroconvective instability near ion-selective surfaces”, in arXiv:


photoassociate

en-verb

photoassociate (third-person singular simple present photoassociates, present participle photoassociating, simple past and past participle photoassociated)

photoassociates (present singular third-person)
photoassociating (participle present)
photoassociated (participle past)
photoassociated (past)

Starting with ultracold #123;87#125;Rb atoms, we apply pulses of frequency-chirped light to first photoassociate the atoms into excited molecules and then, later in the chirp, de-excite these molecules into a high vibrational level of the lowest triplet state, a#92;,#123;3#125;#92;Sigma#95;#123;u#125;#123;#43;#125;.

173003 (2015), J. L. Carini, S. Kallush, R. Kosloff, P. L. Gould, “Enhancement of Ultracold Molecule Formation Using Shaped Nanosecond Frequency Chirps”, in Phys. Rev. Lett., volume 173003:

(physics) To associate atoms by means of photoassociation