「φ」の共起表現(1語右で並び替え) - Weblio英語共起表現検索

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「φ」の共起表現一覧(1語右で並び替え)

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It is a particle of a scalar field	φ; a scalar field that always comes with gravity.
ation of the algebraic relationships between √5,	φ and Φ mentioned above.
when it occurs in combination with two formulas	φ and ψ.
κ is called α-indescribable if for every formula	φ and every subset U of Vκ such that φ(U) holds in
f a golden spiral, and hence are related to both	φ and the Fibonacci series.
ZFC: the embedding j is a class of the form {x \|	φ(x,a)} for some set a and formula φ, and in the l
L in Rn, there are volume-preserving linear maps	φ and ψ from Rn to itself such that
ory which values, or conformations, of the ψ and	φ angles are possible for an amino-acid residue in
Phi Aquarii (	φ Aqr, φ Aquarii) is a star in the constellation A
For this it is necessary that both ψ and	φ are isomorphisms in their respective categories.
Define the constant	Φ as
s the (necessarily finite) maximum value of that	φ attains.
Phi Aurigae (	φ Aur, φ Aurigae) is a star in the constellation A
	φ Aurigae is an orange K-type giant with an appare
Let	φ be an orthogonal wavelet.
uality for 2-positive maps) For a 2-positive map	Φ between C*-algebras, for all a, b in its domain,
The behavior of a point x under the iterates of	φ can be tracked by recording, for each n, the par
icle, respectively, the acoustic contrast factor	φ can be expressed as
e values are known along the wellbore, porosity (	φ) can be inferred by the formula
That is,	φ can be written as a column vector; and so Δφ is
Phi Capricorni (	φ Cap, φ Capricorni) is a star in the constellatio
	φ Capricorni is an orange K-type bright giant with
Phi Centauri (	φ Cen, φ Centauri) is a star in the constellation
With ν and	φ Cen, it marks what has been traditionally portra
	φ Centauri is a blue-white B-type subgiant with an
The new scalar field	φ comes from a component of the metric tensor g55
where	φ denotes all the matter fields.
ctured that logφE comparisons may suffice, where	φ denotes the golden ratio.
Letter	Φ deposited from W(CO)6 by EBID
that the ψ dihedral angle of one residue and the	φ dihedral angle of the next residue sum to roughl
Phi Draconis (	φ Dra / φ Draconis) is a fourth-magnitude star in
Then, if	φ holds, there is an x satisfying φ; but if φ does
sely, if Ω is a critical point of the functional	Φ in a given comohology class and , then Ω defines
and thus our rule 2 needs to be changed so that	φ indicates such a letter or sequence of symbols i
	φ is porosity, dimensionless
where	Φ is the dilaton field.
where	φ is the golden ratio
where	φ is the golden ratio.
The field	φ is consequently dubbed the Liouville field.
where	Φ is a quasi-Newtonian potential given by
The term 2 Ω sin	φ is the Coriolis frequency.
If	Φ is a tautology, and Θ is a substitution instance
e following sentence true when every instance of	φ is replaced by that sequence of symbols: "φ" is
where	Φ is the dilaton, and the equation of motion is
Where A is the vector potential and	φ is the scalar potential.
Namely, if	φ is a Riemann map between D and a second domain E
After this adjustment,	φ is still a flow, and further this adjustment pre
A universal quantification of an open formula	φ is true in a model iff every element in the doma
pascal), k is the permeability (measured in m²),	φ is the porosity (0-1), σ is the surface tension
Mass flux (	Φ) is the rate of mass flow across a unit area (kg
where e is void ratio,	φ is porosity, VV is the volume of void-space (suc
where J is the 3J coupling constant,	φ is the dihedral angle, and A, B, and C are empir
nt wavefunction, proportional to exp(-iφ), where	φ is known as the phase of the wavefunction, this
n existential quantification of the open formula	φ is true in a model iff there is some element in
e a function ψ based on Euler's totient function	φ; it will map positive integers to non-negative i
Define the positive map	Φ: L(H2) → L(H1) by
A linear map	Φ: L(H2) → L(H1) is said to be positive if it pres
	φ maps the root of T1 to the root of T2,
sure test completeness, the domain of a function	φ may be extended with special test inputs that ar
ch (DEAR), kaons were produced by the decay of a	φ meson at the φ factory in DAFNE.
Because it decays into J/ψ and	φ mesons, it has been suggested that this particle
for all L-derivatives,	Φ must hold
Test Completeness: Each processing function	φ must be executable for at least one input, with
tional field), the right hand side vanishes, and	φ obeys the (curved spacetime) wave equation.
The empty subset	Φ of a partially ordered set P is conventionally c
unit vector field uα and two scalar fields σ and	φ, of which only φ is dynamical.
Consider a flow	φ on G and modify it by choosing an edge , reversi
Vary with respect to longitude	φ only to get
f one or a finite number of generating functions	φ or .
Phi Persei (	φ Persei, φ Per) is a Class B2Vpe, fourth-magnitud
Therefore changes in	φ propagate through electrovacuum regions; in this
Phi Piscium (	φ Psc) is a binary star system approximately 380 l
involving cos 2	φ rather than cos2φ -these lead to different numer
rm, then Ω is a critical point of the functional	Φ restricted to the cohomology class .
, given with respect to a Cartesian chart, where	φ satisfies a certain partial differential equatio
Phi Serpentis (	φ Ser, φ Serpentis) is a star in the constellation
language FORMULA-GAME is defined as all formulas	Φ such that Player 1 has a winning strategy in the
It is sometimes marked on camera body with the '	Φ' symbol where the vertical bar represents the ex
The scalar field	φ takes on values in the real vector representatio
th from vacuum, including electron work function	φ that is the depth of Fermi surface from vacuum.
	φ the totient function
and	Φ the cdf of the standard normal distribution.
For a positive value of	φ, the particles will be attracted to the pressure
y observing the angle between the Sun and Earth,	φ, the ratio of the distances to the Sun and Moon
the angular velocity of planetary rotation; and	φ, the latitude.
if we take	Φ to be a propositional formula we can also take ¬
the addition of quantifiers such that if we take	Φ to be a formula of propositional logic and α as
n for Fibonacci numbers linking the nth power of	φ to the nth Fibonacci number.
tern can be calculated by adding the phase shift	φ to the fringing term.
Eliminating	Φ, we get exactly the same equations as before.
Then, in the absence of phases (	Φ), we are unable to complete the shown Fourier tr
rank two tensor field, there is a scalar field,	φ, which has the physical effect of changing the e
tive index n and converging to a spot with angle	φ will make a spot with radius
We have a real scalar field	φ with the following action

共起表現