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Lemma

Market practitioners armed with a term-structure model next need to determine how this relates to the fluctuation of security prices that are related to interest rates. Most commonly, this means determining how the price T of a zero-coupon bond moves as the short rate r varies over time. The formula used for this determination is known as Itos lemma. It transforms the equation describing the dynamics of the bond price P into the stochastic process (4.5). [Pg.70]

The subscripts rr in (4.5) indicate partial derivatives—the derivative with respect to one variable of a function involving several variables. The terms dr and drY are dependent on the stochastic process that is selected for the short rate r. If this is the Ornstein-Uhlenbeck process represented in (4.4), the dynamics of P can be expressed as (4.6), which gives these dynamics in terms of the drift and volatility of the short rate. [Pg.70]

Building a term-structure model involves these steps  [Pg.71]


The following lemma is needed for our result. Consider a matrix Hamiltonian h coupling two states, whose energy difference is 2ra... [Pg.167]

Thus, we still relate to the same sub-space but it is now defined for P-states that are weakly coupled to <2"States. We shall prove the following lemma. If the interaction between any P- and Q-state measures like 0(e), the resultant P-diabatic potentials, the P-adiabatic-to-diabatic bansfomiation maOix elements and the P-curl t equation are all fulfilled up to 0(s ). [Pg.649]

For more than two almost invariant sets one has to consider all eigenmea-sures corresponding to eigenmodes for eigenvalues close to one. In this case, the following lemma will be helpful. [Pg.106]

Lemma 3. Let p M be a probability measure and let X and Y be disjoint sets which are dx- resp. dy-almost invariant with respect to p. Moreover suppose that f (X) n Y = 0 and f Y) n A = 0. Then X UY is 6xuy-almost invariant with respect to p where... [Pg.106]

This approximation is a special case of the Baker-Campbell-Hausdorff lemma for additional discu.ssion and extensions to more general classes of methods. [Pg.353]

Lemma 1.1. For every convex and differentiable functional J the function... [Pg.24]

The right-hand side is nonnegative here in view of (1.61), therefore (A) > 0. Lemma 1.1 is proved. [Pg.24]

Taking into account Lemma 1.1, we conclude that the left-hand side of this inequality converges from above to J(,(uo — u)- Thus... [Pg.25]

By (1.97), the right-hand side is nonnegative, which proves the assertion. Lemma 1.4. The following estimate takes place ... [Pg.36]

The proof of this theorem is based on the following lemmas. [Pg.37]

By making use of the strong monotonicity of A, Holder s inequality, and Lemma 1.2, we obtain the estimate... [Pg.40]

Applying Holder s inequality and using the strong monotonicity of A, the monotonicity of / , Lemma 1.2 and the estimates for the norms, we obtain... [Pg.41]

This inequality reduces to the estimate (1.122) and completes the proof. From Lemma 1.9 the following assertion is immediately deduced. [Pg.45]

Take the norm of both parts of this equality and use the Lipschitz continuity of P (see Lemma 1.2). By the linearity of I, it provides... [Pg.47]

Lemma 1.12. If the boundary dflc belongs to the class and a function u G iF (f2c) is given, then the normal derivatives at the boundary dflc are uniquely defined. [Pg.51]

Proof. By utilizing the local coordinate systems (1.135), the assertion of Lemma 1.13 reduces to the case... [Pg.52]

By Lemmas 1.12, 1.13 and property (1.137), from Theorem 1.24 the next statement follows. [Pg.54]


See other pages where Lemma is mentioned: [Pg.565]    [Pg.565]    [Pg.565]    [Pg.113]    [Pg.24]    [Pg.36]    [Pg.36]    [Pg.36]    [Pg.36]    [Pg.37]    [Pg.38]    [Pg.38]    [Pg.38]    [Pg.38]    [Pg.38]    [Pg.39]    [Pg.39]    [Pg.44]    [Pg.44]    [Pg.46]    [Pg.46]    [Pg.47]    [Pg.47]    [Pg.47]    [Pg.51]    [Pg.52]    [Pg.53]    [Pg.54]    [Pg.54]    [Pg.55]    [Pg.63]    [Pg.64]    [Pg.65]    [Pg.65]   
See also in sourсe #XX -- [ Pg.738 ]

See also in sourсe #XX -- [ Pg.9 , Pg.76 , Pg.79 , Pg.306 ]

See also in sourсe #XX -- [ Pg.252 ]

See also in sourсe #XX -- [ Pg.252 ]

See also in sourсe #XX -- [ Pg.43 , Pg.44 ]

See also in sourсe #XX -- [ Pg.109 , Pg.115 ]




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A-lemma

Auxiliary Lemmas

Barbalat’s Lemma

Bounded Functors Way-Out Lemma

Cauchy Lemma

Closing lemma

Definitions and Schurs Lemma

Factorization lemma

Fundamental Lemma

Gluing lemma

Homotopy lemma

Inversion lemma

Ito’s lemma

Lemma Cauchy-Frobenius

Lemma primordia

Lorentz lemma

Lorentz lemma and reciprocity relations

Morse lemma

Nakayama s lemma

Nerve lemma

Neyman-Pearson Lemma

Noether normalization lemma

Notations and Basic Ideas. Auxiliary Lemmas

Poincare lemma

Projection lemma

Properties and Lemmas

Pumping lemma

Quillen lemma

Racah’s lemma

Schur s lemma

Schurs Lemma

Splitting lemma

The Noether Normalization Lemma

Two Lemmas

Yoneda lemma

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