Sheep's vool shtickin' by der fences efferwhere on der ranch, py cosh!
"Flying U Ranch" by B. M. Bower
Und py cosh, I use him too if dem fellers coom by us mit der dry farms alreatty!
"The Flying U's Last Stand" by B. M. Bower
In his left pocket there was a cosh and in his right a revolver.
"Tartarin de Tarascon" by Alphonse Daudet
M'Cosh ain't been seen for four or five days.
"The Nether World" by George Gissing
By cosh, dem bodadoes iss sell high.
"North of Fifty-Three" by Bertrand W. Sinclair
The Sioux counted their money by dimes, which they called Cosh-poppy.
"Old Rail Fence Corners" by Various
I shouted wildly to Cosh to toss me one from near by.
"The Escape of a Princess Pat" by George Pearson
Copeland, Cosh, and M'Nair, along with their respective wives.
"The Story of John G. Paton" by James Paton
Robert Cosh, what have ye to say?
"Young Barbarians" by Ian Maclaren
Mr. M'Cosh touched his cap and crossed to the other side of the deck.
"A Marriage at Sea" by W. Clark Russell
I'd carry the cosh meself if I'd got a woman like 'er.
"A Child of the Jago" by Arthur Morrison
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Can they be my lassocks—ance cozie an' cosh,
Weel shapit, weel happit—sae stumpy an' tosh?
Twa coats an' a toush, or a goon, ye may ween,
Were boukie aneuch, wi' what nature had gi'en.
"Crinoline" by Janet Hamilton
O false SIR JOHN KANE! is it thus that you praych me?
I think all your Queen's Universitees Bosh;
And if you've no neetive Professor to taych me,
I scawurn to be learned by the Saxon M'COSH.
"The Last Irish Grievance" by William Makepeace Thackeray
As I think of the insult that's done to this nation,
Red tears of rivinge from me fatures I wash,
And uphold in this pome, to the world's daytistation,
The sleeves that appointed PROFESSOR M'COSH.
"The Last Irish Grievance" by William Makepeace Thackeray
Since all the switches are completely uncorrelated, the original formula for Σ–potential, Eq. (3), results in the following expression for Ξ(X ): Ξ = N+κ log[cosh(2X− )].
Generalized Entropy approach to far-from-equilibrium statistical mechanics
The replica-symmetric order-parameter function may thus be written as exp {βx Pa σa + βy Pa σa τ a + β z Pa τ a } c(σ , τ ) = Z dx dy dz P (x, y , z ) [2eβy cosh (β (x + z )) + 2e−βy cosh (β (x − z ))]n , where the denominator serves to normalize R dx dy dz P (x, y , z ) = Pσ ,τ c(σ , τ ).
Metastable configurations of spin models on random graphs
The fourvelocity ﬁeld of our solutions thus becomes uµ = (cosh η , 0, 0, sinh η ).
Simple solutions of relativistic hydrodynamics for longitudinally expanding systems
The fourmomentum of the observed particles with mass m is denoted by kµ = (mt cosh y , kx, ky , mt sinh y ).
Simple solutions of relativistic hydrodynamics for longitudinally expanding systems
Longitudinal boostinvariance dictates freeze-out along a surface of ﬁxed longitudinal proper time τf (x⊥ ), and we can write Σµ (x) = (cid:0)τf (x⊥ ) cosh η , x⊥ , τf (x⊥ ) sinh η(cid:1).
Elliptic Flow from a Transversally Thermalized Fireball
For massive particles we must generalize Eq. (5.3) by writing the ﬁrst term as m⊥ cosh(y−η) and use k · u = γ⊥ (cid:0)m⊥ cosh(y−η) − k⊥ ·v⊥ (cid:1).
Elliptic Flow from a Transversally Thermalized Fireball
Eε / cosh(c|.|) and gα ε,x (y ) := ∂ αfε (y ) cosh(c|x − y |).
Elliptic regularity and solvability for partial differential equations with Colombeau coefficients
After the phase shift the modes are ampliﬁed by the factor cosh(Θ/2) and mixed, with the overlap sinh(Θ/2), and ﬁnally the outgoing modes gain the absolute phase Ψ/2 and the relative phase Λ.
Quantum Physics of Simple Optical Instruments
Figure 2: Comparaison of the threshold of instability for the full equation (9) (crosses) with the theory obtained from (14) with α = −1 for u1 = A exp[−K x] (full line left ﬁgure) and u1 = A/ cosh(K x) (full line right ﬁgure).
Nonlinear supratransmission as a fundamental instability
The eigenvalues are given by λρ (n) = h[2 cosh(β J )]n tanhρ (β J )iJ , and it is clear that the largest corresponds to ρ = 0.
Diagonalization of replicated transfer matrices for disordered Ising spin systems
It is enough to consider explicitly the case x > 2 and parameterize x = 2 cosh φ, φ < ∞.
Introduction to the Random Matrix Theory: Gaussian Unitary Ensemble and Beyond
Calculation of the Integral over Q. (8.51) we use the parameterization Q = et er cosh s e−iθ sinh s e−r cosh s ! .
QCD, Chiral Random Matrix Theory and Integrability
We ﬁrst perform the integral over r , which gives a factor 2K0 (2N ǫ cosh s cosh t) with leading singularity given by ∼ − log ǫ.
QCD, Chiral Random Matrix Theory and Integrability
Note that since (e, p) = (m cosh θ, sinh θ), we have to replcae, accordingly, θ → iπ/2 − θ.
Bosonic Theory with a Random Defect Line
Backlund ﬁeld , and from the matrix model point of view, where µB is the eigenvalue coordinate, σ is essentially the “time of ﬂight variable.” For the different branes µB ∼ p|µ|coshσ or µB ∼ p|µ|sinhσ .
Observations On The Moduli Space Of Two Dimensional String Theory
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