In literature:
WASHINGTON, June 21 1862 6 PM.
"The Papers And Writings Of Abraham Lincoln, Volume Six" by Abraham Lincoln
WASHINGTON, June 21 1862 6 PM.
"The Papers And Writings Of Abraham Lincoln, Complete" by Abraham Lincoln
On May 10, 1944 they opened the bar at 6 pm and Bruce and I ordered a glass of Scotch and a beer each.
"The Biography of a Rabbit" by Roy Benson
Take the point P where the two curves meet, and draw the perpendicular PM to meet OX.
"Supply and Demand" by Hubert D. Henderson
EP is the normal, and the actual motion of P is PM, perpendicular to EP, the angle PEM being made equal to CEA.
"Scientific American Supplement, No. 595, May 28, 1887" by Various
All artificers and laborers hired by the day or week shall work from 5 am to 7 PM.
"Our Legal Heritage, 5th Ed." by S. A. Reilly
Pm sorry he spoke to you like that, for I'm sure you'll be tired and weary.
"The Pilots of Pomona" by Robert Leighton
At 4 PM we filed out of the city.
"By Canoe and Dog-Train" by Egerton Ryerson Young
Ignoring this assured the PM we would get a more definite date from her during the week.
"Greener Than You Think" by Ward Moore
Saw the Sloop and Brig about 5 PM.
"Privateering and Piracy in the Colonial Period" by Various
But as I tol' you, we got to be doin' some'pm.
"Sube Cane" by Edward Bellamy Partridge
Started about two pm, and rattled through Oxford, only stopping here and there to do our shopping.
"The Cruise of the Land-Yacht "Wanderer"" by Gordon Stables
The dental formula of the first is I (1 or 0)/3 C 1/1 Pm 4/4 M 2/2 = 34 or 36, of the latter I 3/3 C 1/1 Pm 4/4 M 2/2 = 40.
"The Cambridge Natural History, Vol X., Mammalia" by Frank Evers Beddard
Let PM and QN be those ordinates of the curve which have M and N as their feet.
"Encyclopaedia Britannica, 11th Edition, Volume 14, Slice 5" by Various
BRITISH COLUMBIA: Vermilion Crossing, Kootenay, 1 (ROM); Paradise Mine, 3 (PM); Crows Nest Pass, 4450 ft., 3 (NMC); Newgate, 10 (NMC).
"North American Jumping Mice (Genus Zapus)" by Philip H. Krutzsch
***
In news:
Sat, Dec 8: 12:40 pm 3:10 pm 5:35 pm 8:10 pm 10:30 p.m.
Performances are scheduled for 7 pm Friday, 2 and 7 pm Saturday and 2 pm Sunday, Nov 16-18, at Bremer Theater.
30 pm Wednesday-Thursday, 8 pm Friday-Saturday, 2 pm Saturday Civic Center Music Hall 201 N Walker lyrictheatreokc.com, 524-9312 $31-$60.
Regular hours will be from 4 to 7 pm Monday through Friday, 10 am to 7 pm on Saturday, and 1 to 5 pm on Sunday.
Monday 8 am - 5 pm (Closed 12 pm - 1 pm lunch).
Visitation will be from 9 am to 5 pm, Saturday, Nov 3, and from 1 to 7 pm, Sunday, Nov 4, at Cooper Funeral Home and the family will gather from 4 to 6 pm to meet with friends.
Fri, Dec 7: 12:00 pm 2:20 pm 4:40 pm 7:10 pm 9:35 p.m.
Sat, Dec 8: 12:00 pm 2:20 pm 4:40 pm 7:10 pm 9:35 p.m.
Showtimes are tonight, Nov 16, at 7 pm and Saturday, Nov 17, at 7 pm and Sunday, Nov 18 at 2 pm, all at the Oak Bluffs School.
The performances, by elementary students and middle schoolers at SCAPA, will be at 8 pm Friday, and 2 pm and 8 pm Saturday at the Opera House.
Anna Karenina (R) Fri 1 pm, 4 pm, 7 pm, 10 pm.
Argo (R) Thurs 2 pm, 5 pm, 8 pm.
Breaking Dawn Part 2 (PG-13) Thurs 12:45 pm, 1:30 pm, 2:45 pm, 3:30 pm, 4:15 pm, 5:30 pm, 6:15 pm, 7 pm, 8:15 pm, 9 pm, 10 pm.
Wreck-It Ralph (PG) Thurs 12:30 pm, 1:45 pm, 3 pm, 4:15 pm, 6:45 pm, 9:15 pm.
The Collection (R) Thurs 1:15 pm, 3:40 pm, 6:15 pm, 8:30 pm, 10:45 pm.
***
In science:
On the manifold X we have ∂ θ ⊗ α, where ∂b = Pm j=1 ϑj ⊗ Zj and ¯∂b = Pm d = ∂b + ¯∂b + ∂ ¯ϑj ⊗ ¯Zj .
Universality and scaling of zeros on symplectic manifolds
H }(τ ), δpm (τ ) = µ(τ ){pm , H }(τ ), This local symmetry may be ﬁxed by implying the gauge condition ˙λ = 0 ⇒ ¨µ = 0 after that only global modes of gauge transformations survive µ(τ ) = ν1 τ + ν2 .
Point particle in general background fields and generalized equivalence principle
P (D) such that Pm (ξ0 ) is invertible in eC for some in ξ0 ∈ Rn where Pm (ξ ) denotes the principal part.
Elliptic regularity and solvability for partial differential equations with Colombeau coefficients
We will denote the group (pM , H ) by Γ(pM ).
On linearity of finitely generated R-analytic groups
Each step of the calculation in the case of operators ˆq n′ ◦ ˆp m′ , ˆq n′′ ◦ ˆp m′′ and ˆq n′′′ ◦ ˆp m′′′ has the corresponding one in the c-number case for qn′ · pm′ , qn′′ · pm′′ and qn′′′ · pm′′′ which satisfy the Jacobi identity.
Weyl ordering rule and new Lie bracket of quantum mechanics
Galaxy clusters have very small mean magnetic ﬁelds, little rotation and thus little helicity, a nd very large magnetic Prandtl number Pm , where Pm = n/h, n is the viscosity,7 and h is the resistivity.
Thermal conduction and particle transport in strong MHD turbulence, with application to galaxy-cluster plasmas
We call the PM such obtained the geometric PM .
Patterns of the ground states in the presence of random interactions: nucleon systems
Equivalently, we can think of Pm as a set of equivalence relations on Nm and write i ∼π j if i and j belong to the same interval of π ∈ Pm .
Balls-in-boxes duality for coalescing random walks and coalescing Brownian motions
We shall say that K ∈ L1 (µ; L(H, Y )) has ﬁnite rank if for some m ∈ N, K = Pm k=1 hj ⊗ yj with uj ∈ L1 (µ; H ) and yj ∈ Y , that is, Kh = Pm j=1 (uj , h)yj .
The Clark-Ocone formula for vector valued random variables in abstract Wiener space
Then in a characteristic φ- ˇSerstnev PN space (V , ν, τ , τ ∗ ) if pm −→ p in V and A = {pm : m ∈ N}, then A is a D-bounded subset of V .
Some results in Generalized \v{S}erstnev spaces
Now {pm} is a subset of D-compact set A, so it has a convergent subsequence {pm}m∈J ′ .
Some results in Generalized \v{S}erstnev spaces
In what follows, we will assume we have performed such a rescaling to a natural variable y, and that ZN is deﬁned by eq. (15), with H (z) = (cid:229)m pm zm taken to generate a desired degree distribution { pm }.
Random Feynman Graphs
Pm is the matrix (∆Pm )x,x+ei = ∆m(x, x + ei ) (and null anywhere else).
Random walks in a Dirichlet environment
Q = [qij ], (0 ≤ j ≤ pM − 1, 0 ≤ i ≤ pM − 1), the matrix of transition probability intensities of the process {XM (t), t ≥ 0} has Parisi matrix form.
Random walk on p-$adics in glassy systems
If x, y ∈ V are such that x 6= y and x ↔ y in m then, for A ⊆ V , PM(cid:0)∂N = {x, y}, ∂ (M \ N) = A(cid:1) = PM(cid:0)∂N =
Flows and ferromagnets
***