He had once been famous for his soapy manners: now he was as rough as a Highland stot.
"The Moon Endureth--Tales and Fancies" by John Buchan
I've killt mony a stot like it, shoost t' keep in the way of it.
"The Yeoman Adventurer" by George W. Gough
But the stot didn't mean to be gaffed.
"Prince Fortunatus" by William Black
We'll sune hae neither cow nor ewe, We'll sune hae neither staig nor stot.
"Ballads of Scottish Tradition and Romance" by Various
Foiled in this direction, I worried the President, as old Mustard would a stot, until he wrote the permission so long solicited.
"Destruction and Reconstruction:" by Richard Taylor
That maun be a College-bred stot, from the way he behaves.
"The House with the Green Shutters" by George Douglas Brown
Auld stots hae stiff horns.
"The Proverbs of Scotland" by Alexander Hislop
I'm getting tired o' bear-beef, and wouldn't mind a slice out of a juicy stot's rump.
"Wild Adventures round the Pole" by Gordon Stables
Quartus fuit Robertus Stot qui eciam mortuus est sine herede.
"Villainage in England" by Paul Vinogradoff
Little does she know that WILLIAM STOTT of Oldham has stotted her down in his note-book.
"Punch, or the London Charivari, Volume 93, December 24, 1887" by Various
***
S z tot = 0, the obtained target states generally have the ﬁnite total spin Stot .
Low Energy Properties of the Random Spin-1/2 Ferromagnetic-Antiferromagnetic Heisenberg Chain
As we will show in short, the mathematical identity he−R i = 1, together with Eq. (7), implies the following integral ﬂuctuation theorem for the total entropy variation along a stochastic tra jectory ∆stot, he−∆stot i = 1.
Test of the fluctuation theorem for stochastic entropy production in a nonequilibrium steady state
S (t) is the contribution to ˙Stot (t) coming from the changes in the system probability distribution and ˙Sr (t) is the contribution coming from matter and energy exchange processes between the system and its reservoirs.
Entropy fluctuation theorems in driven open systems: application to electron counting statistics
We next summarize our results ˙Stot (t) = ˙Sna (t) + ˙Sa (t) ≥ 0 ˙Sna (t) = ˙Sd (t) + ˙Sb (t) ≥ 0 ˙Sa (t) ≥ 0 .
Entropy fluctuation theorems in driven open systems: application to electron counting statistics
The long time limit is needed in order to neglect the contribution from ∆s[m(τ ), t] to ∆stot [m(τ ), t].
Entropy fluctuation theorems in driven open systems: application to electron counting statistics
Fig. 2c shows the time dependent EP ˙Stot and its adiabatic ˙Sa and nonadiabatic contribution ˙Sna .
Entropy fluctuation theorems in driven open systems: application to electron counting statistics
We see that at steady state ˙S = 0 so that ˙Stot = ˙Sr .
Entropy fluctuation theorems in driven open systems: application to electron counting statistics
The structure of P (∆Stot ) can be understood using P (∆Sr ) and P (∆S ) because ∆stot = ∆sr + ∆s.
Entropy fluctuation theorems in driven open systems: application to electron counting statistics
Given these assumptions we can ask for what partition will Stot be maximum, or equivalently, which partition is the most probable? If we write E2 = Etot − E1 and recall that Etot is ﬁxed, this task is easy.
Making Sense of the Legendre Transform
The von Neumann entropy of the total system is clearly zero Stot = −tr ρtot log ρtot = 0.
Holographic Entanglement Entropy: An Overview
Thus, the functional Stot [A, λ, c, ¯c, b; A∗, λ∗, c∗ ; ξ, µ, ε] which solves both the ghost equation (2.24) and the gauge-f ixing condition (2.23) has the form Stot = Z d4x (b + ξ · ∂ ¯c)niAi + ¯S [A, λ, c; ˆA∗ i, A∗J, λ∗, c∗ ; ξ, µ, ε], where the b-dependent term ensures the validity of condition (2.23).
Gauge Theories on Deformed Spaces
The Ward identities describing the (non-)invariance of Stot under the VSUSY variations δi, the vectorial symmetry transformations ˆδi and the translations ∂i can be derived from the ST identity (2.22) by dif ferentiating this identity with respect to the corresponding constant ghosts εi, µi and ξ i, respectively.
Gauge Theories on Deformed Spaces
The spin quantum number in this phase is given by Stot = (L − Nc )/2, where L is the number of lattice sites and Nc the number of conduction electrons.
One Dimensional Kondo Lattice Model Studied by the Density Matrix Renormalization Group Method
The total ﬂux Stot in this ﬁlter depends on the same exposure factor and on ∆λ, so that the Stot ∝ 1/n2 and σtot ∝ 1/n.
Object Classification in Astronomical Multi-Color Surveys
Within this description, the total spin of the system is Stot (q) = s(q) + S(q).
Ward identities for strongly coupled Eliashberg theories
***