Another posts

words with muse in them helioscope definition bos taurus definition wind etymology marble hearted snuff mulls bartholomeu dias definition centauromachy definition the road to heaven is paved with miles of clouded hell assay ton geometric lathe definition of eleutheromania martel de fer thrown off guard tactile sensation definition agnatha definition xenium definition here and there definition calculus etymology postcentral gyrus definition weaver hitches inconsumable definition hieratic script definition trisagion definition coal box corozo palm vasty definition allocatur definition clarifiers definition vestiture definition pin hold vastly define define unburnished shied away definition connaught brogue



  • WordNet 3.6
    • n TDT (astronomy) a measure of time defined by Earth's orbital motion; terrestrial time is mean solar time corrected for the irregularities of the Earth's motions
    • ***


In news:

In the 21st century his evening-length works have supplanted TDT's earlier tradition of presenting mixed bills drawn from the repertoire.
It's also a four-parish bicycle tour, a kayak and canoe race for kids, an adult TDT "prelim" in the spring, a day camp for teens and a bayou cruise for Man's Best Friend.

In science:

Bt + ∇b(xt )γtdt and starting from γ0, where B is a Brownian motion and σ(x)σ(x)∗ = a(x).
Structure of large random hypergraphs
C ε1 · βl e−βl tdt on [−R, R] (and zero otherwise). ii.
On a nonhierarchical version of the Generalized Random Energy Model. II. Ultrametricity
Beta(p, q |α, β ) where Γ(α) = R ∞0 tα−1 e−tdt is the Gamma function.
Exact Non-Parametric Bayesian Inference on Infinite Trees
In this case, the pdf N ft(x) (1 − Ft (x))N −1 tends to a point mass at the N ft (x) (1 − Ft (x))N −1 tdt minimum of t and the integral approaches the minimum of t.
Modulation Codes for Flash Memory Based on Load-Balancing Theory
We shall work on L2 (R, dt) on each Fourier mode, which amounts to conjugating by et/2 to pass unitarily from L2(e−tdt) to L2 (dt): let eKh := et/2Khe−t/2 and eKh,k its decomposition on the k Fourier mode fk (t) of f (t, y ).
Random walk on surfaces with hyperbolic cusps
To implement this behavior, we use the approximation Rm (z = 1 − ǫ) ≃ Rm (∞)/ǫ + R tx 1 (Rm (t) − Rm(∞))e−ǫtdt, and determine the leading behavior of Rm (z ) by comparing different time scales ǫ−1, tc, and tx .
First passage time for random walks in heterogeneous networks
Wt = W [(µρtdt + σρt dBt − γF (f )dt)] dρt = (cid:2)f + ρt (1 − ρt )(µ − σ2ρt )(cid:3) dt + [σρt (1 − ρt )] dBt + γ ρtF (f )dt For a derivation of these equations, see .
Optimal hedging of Derivatives with transaction costs
TDT) (38), but that otherwise two offspring are required.
1953: An unrecognized summit in human genetic linkage analysis
TDT (38) and other family-based association tests that may be the best hope for mapping the genes associated with complex traits.
1953: An unrecognized summit in human genetic linkage analysis
Proof: The proof makes use of the Gaussian integration by parts formula EdXσ (t)f (cid:18)Z dXσ′ (s)(cid:19) = Ef ′ (cid:18)Z dXσ′ (s)(cid:19) Z EdXσ (t)dXσ′ (s) = Ef ′ (Xσ′ ) 1IA( dist(σ,σ′ ))≥tdt where f is any differentiable function.
Rigorous results on some simple spin glass models
Fix a point realization D = L∞ (X, µ), and set XD := X × R equipped with the usual product measure dµ ⊗ e−tdt and F D t (x, s) := (x, s + t).
Amalgamated free product over Cartan subalgebra, II. Supplementary results & Examples
Ei (z) = − R ∞ −z e−tdt/t is the exponential integral function, and where the principal value of the integral must be taken.
Reheating the Universe in Braneworld Cosmological Models with bulk-brane energy transfer
Et × {t} is a measurable subset of Ω × [0, ∞) such that XE ∈ Ω XE (t) dx = m0 for al l t ≥ 0, and XE |t=0 = XE0 in L1 (Ω). (3) V is a Radon measure on Ω × Gd−1 × (0, ∞) such that V = V tdt where V t is for almost al l t ∈ (0, ∞) a general varifold on Ω, i.e., a Radon measure on Ω × Gd−1 .
Existence of weak solutions for a non-classical sharp interface model for a two-phase flow of viscous, incompressible fluids
M 2 V (m2, t) tanh(πt)tdt + O(T −A ) with A arbitrarily large.
Bounds for $GL(3)\times GL(2)$ $L$-functions and GL(3) $L$-functions
PtT = rtPtT dt + ΩtT PtT (dWt + λtdt), Here PtT is the random value at time t of the bond that matures at time T, {rt}t≥0 is the short rate, {ΩtT }T ≥t≥0 is the bond volatility, and {λt}t≥0 is the market price of risk.
Rational term structure models with geometric Levy martingales