It is often largely admixed with essence of turpentine.
"Scientific American Supplement, No. 799, April 25, 1891" by Various
It is preferable to feed meal admixed with cut fodders.
"Pratt's Practical Pointers on the Care of Livestock and Poultry" by Pratt Food Co.
This consisted of synovial fluid admixed with a varying proportion of blood.
"Surgical Experiences in South Africa, 1899-1900" by George Henry Makins
This product has been admixed with soap for many years, the quantity generally used being about 5 per cent.
"The Handbook of Soap Manufacture" by W. H. Simmons
Admixed was a sincere aim to establish free political conditions.
"History of the Great American Fortunes, Vol. I" by Myers Gustavus
The stronger this is the more it will colour the performance, when unconsciously admixed.
"Piano Playing" by Josef Hofmann
Wood ash was admixed with the clay.
"The Cultural History of Marlborough, Virginia" by C. Malcolm Watkins
The high toxicity of barium was called attention to by early observers, but it was attributed by some to admixed arsenic.
"Barium, A Cause of the Loco-Weed Disease" by Albert Cornelius Crawford
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Here H0 and V may belong to a same symmetry class, with √Y − Y0 governing the parametric eigenvalue dynamics, or different symmetry classes with √Y − Y0 as a parameter for symmetry admixing transitions.
Random Matrices with Correlated Elements: A Model for Disorder with Interactions
The spin-ﬂip matrix element of ˆHe−ph is nonzero due to the admixing of the upper ψnℓz (ρ) |si states to the ground state ˜ψgrρ) |˜si , where |˜si shows that spin is an approximate quantum number due to the SO coupling.
Spin relaxation in quantum dots with random spin-orbit coupling
On the other hand, his calculations may not be ideal for this problem because his model admixes into a homogeneous ISM the same fraction for each supernova’s ejecta (a= 1.7×10−5) after Monte Carlo sampling to obtain N=70 supernovae.
Are Ti44-Producing Supernovae Exceptional?
The physical result would be that virtual transitions to the excited states lead to an admixing of those states with the low-energy sector.
Effective Spin-1/2 Description of Transverse-Field-Induced Random Fields in Dipolar Spin Glasses with Strong Single-Ion Anisotropy
We denote by Wkµ the square of the amplitude with which an unperturbed shell–model conﬁguration labeled µ is admixed into an eigenstate of the shell–model Hamiltonian.
Random Matrices and Chaos in Nuclear Physics
If that mixing time is small or at most of the order of the time it takes to excite the DGDR from the GDR, then each of the background states admixed to the GDR mode may get excited into its own GDR.
Random Matrices and Chaos in Nuclear Physics
The measurements are performed on individual oscillation lines of carbon dioxide laser for nitrogen flow admixed by ammonia (13.6 ppm) [30,31].
Small-Size Resonant Photoacoustic Cell of Inclined Geometry for Gas Detection
Thus, it will “stick out,” as its description along its one axis in the vector space will likely not be well-expressed in terms of the other axes, i.e., in terms of the other SNPs, and by the time it “works its way back” due to population admixing, etc., other SNPs will have occurred elsewhere.
Randomized algorithms for matrices and data
The purity of the intrinsic part becomes perfect when γev ≫ Γs ; the depletion of admixed states of the opposite isospin occurs faster than their population.
A Simple Mode on a Highly Excited Background: Collective Strength and Damping in the Continuum
The isospin purity is restored because of the very fast depopulation of the admixed background states when their decay width γev increases compared to the spreading width Γs of the simple state (IAS in this case).
A Simple Mode on a Highly Excited Background: Collective Strength and Damping in the Continuum
The theory is renormalizable and we see that monomial operators ϕℓ′ of dimension not greater than the dimension of the monomial ϕℓ are the only ones admixing to the blocked operator {ϕℓ}k→0 with UV divergent coeﬃcients.
Renormalization of composite operators
While the extent of such isospin admixing is expected to be smaller than the total mixing due to isospin non-conserving terms [6, 10, 11, 13, 43], it may inﬂuence precise model calculations depending on the importance of the charge dependence in pairing correlations.
Isospin symmetry breaking in an algebraic pairing Sp(4) model
One could isolate this term by an isospin analysis of a complete set of PNC NN observables or, alternatively, by ﬁnding a case in which the isospins of the admixed nuclear states select only the ∆I=1 contribution Unfortunately, experimental progress in this ﬁeld has been slow.
Fundamental Symmetries and Conservation Laws
Small contributions from the energies of admixed core states are not shown. ∆Ec is the contribution of the nuclear core level spacing; the values of ∆Ec are taken from experiment.
Strangeness nuclear physics: a critical review on selected topics
Hence the quantity ξe speciﬁes the greatest possible number of eigenstates, where the basis state |0i can be effectively admixed.
Ergodic Properties of Local Spectral Density for a Conservative System of Coupled Quantum States
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