Problem Set 7 - Mathematical Physics | Physics 212A, Assignments of Physics

Material Type: Assignment; Class: MATH PHYSICS; Subject: Physics; University: University of California - Irvine; Term: Unknown 1989;

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Problems, set 7. PHYSICS 212A: Mathematical Physics
1. Using integration by parts, find asymptotic series of the integral for x ,a > 0:
F(x, a) = Z
0
ext
t+adt
Write down the nth term of the series, ϕn(x), (numerate term of the series from n= 0).
Obtain the remainder term Rn(x) explicitly and find the upper bound on its magnitude.
Show that |Rn(x)n(x)| 0 as x .
2. Expansion under integral as a modified Laplace method.
The complimentary error function erfc(x) can be re-written as:
erfc(x) = 2
πZ
x
exp(t2)dt =2
πexp(x2)Z
0exp(2tx) exp(t2)dt
The “straightforward” Laplace’s method cannot be applied since the maximum of the function
in exponential is outside of the range of integration [find where], so the function is maximal
at the end point; also the slope of the exponent function is not zero at this end point.
Nevertheless, one can apply the ideology of the Laplace’s method here since the contribution
of the integrand tends to be confined to the neighborhood of the end point as x+.
Expanding exp(t2) in a power series around the end point, integrate the above expression
term by term to obtain an asymptotic expansion for large x. Write 4 non-zero terms. Obtain
explicitly the nth term of such an expansion, (with the first term in expansion corresponding
to n= 0). Write down explicitly the convergence test. Show whether this asymptotic series
is converging or not.
3. M&W: 3-35, leading term of the expansion only.
4. Use method of stationary phase to find leading behavior, valid as x+, of the integral
I(x) = Z1
0exp µix µ1sin t
t¶¶ dt
Hint. After expanding the function in exponential about its extremum extend the upper limit
of integration to .
5. Using the saddle-point method, find leading behavior of the integral valid for u+
I(u) = Z
−∞
dx
2πsin(x2+ux)
Hint. Change sine to exponent, then xz. Identify saddle point(s) of the function in
exponential. Bend the contour so it goes through the saddle point in the “correct” way.
6. [Extra credit problem. Part of the credit will be given for completing part (a)].
Use the Laplace’s method to obtain (a) the leading term only, (b) the first three terms of the
asymptotic expansion of the integral, for n+
In=Z1
1(1 x2)ndx
pf2

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Problems, set 7. PHYSICS 212A: Mathematical Physics

  1. Using integration by parts, find asymptotic series of the integral for x → ∞, a > 0:

F (x, a) =

∫ (^) ∞

0

e−xt t + a

dt

Write down the nth term of the series, ϕn(x), (numerate term of the series from n = 0). Obtain the remainder term Rn(x) explicitly and find the upper bound on its magnitude. Show that |Rn(x)/ϕn(x)| → 0 as x → ∞.

  1. Expansion under integral as a modified Laplace method. The complimentary error function erfc(x) can be re-written as:

erfc(x) =

π

∫ (^) ∞

x

exp(−t^2 )dt =

π

exp(−x^2 )

∫ (^) ∞

0

exp(− 2 tx) exp(−t^2 )dt

The “straightforward” Laplace’s method cannot be applied since the maximum of the function in exponential is outside of the range of integration [find where], so the function is maximal at the end point; also the slope of the exponent function is not zero at this end point. Nevertheless, one can apply the ideology of the Laplace’s method here since the contribution of the integrand tends to be confined to the neighborhood of the end point as x → +∞. Expanding exp(−t^2 ) in a power series around the end point, integrate the above expression term by term to obtain an asymptotic expansion for large x. Write 4 non-zero terms. Obtain explicitly the nth term of such an expansion, (with the first term in expansion corresponding to n = 0). Write down explicitly the convergence test. Show whether this asymptotic series is converging or not.

  1. M&W: 3-35, leading term of the expansion only.
  2. Use method of stationary phase to find leading behavior, valid as x → +∞, of the integral

I(x) =

∫ (^1)

0

exp

( ix

( 1 −

sin t t

)) dt

Hint. After expanding the function in exponential about its extremum extend the upper limit of integration to ∞.

  1. Using the saddle-point method, find leading behavior of the integral valid for u → +∞

I(u) =

∫ (^) ∞

−∞

dx 2 π

sin(x^2 + ux)

Hint. Change sine to exponent, then x → z. Identify saddle point(s) of the function in exponential. Bend the contour so it goes through the saddle point in the “correct” way.

  1. ∗[Extra credit problem. Part of the credit will be given for completing part (a)]. Use the Laplace’s method to obtain (a) the leading term only, (b) the first three terms of the asymptotic expansion of the integral, for n → +∞

In =

∫ (^1)

− 1

(1 − x^2 )n^ dx

With Mathematica, check the accuracy of the asymptotic results of (a) and (b) for n = 2. Hints. Rewrite the integrand as an exponent of a function. For (a), expand the exponential function near extremum, then show that the limits can be extended to ±∞. For (b), change the variables x → s so the integrand becomes f (s)e−s 2 , same change should ensure the limits extend to ±∞. Expand the prefactor f (s) up to the order needed and integrate term by term.

  1. An ingenious method of finding asymptotic series is discussed in M&W, pp. 89-90(1), that combines the “advanced” methods with the “direct” ones: after the leading term is obtained (via the saddle-point, e.g.), the subsequent terms represent a power series with unknown coefficients; then one can use the recursion relation to match such power series in the r.h.s. and l.h.s. of the recursion relation term by term, reducing the problem to a set of simple (linear) algebraic equations. Consider the derivation of the series for Γ(z + 1) in M&W. Redo the algebra in Mathematica, keeping terms up to

z^25

. Obtain all the terms upto this order. Observe that the coefficients increase after initial decrease, indicating the series is asymptotic. Hints. Use a[i] instead of A, B, etc. for the coefficients. Use Sum[a[i]/(z+1)i, ...] to generate the unknown power series. Using Series[f(z),{z,Infinity,n}] gives an expansion in powers of 1/z to order n. Normal[...] truncates the series (no O(1/z(n+^1 ))). Coefficient[f,1/z,i] produce coefficient of 1/zi^ in f. Using Solve on the set of equations one can equate all the coefficients in the two series. Using Table[...] one can create a list of equations to be solved.

(^1) from after Eq. 3-86 to the end of the Chapter (for possible variations in the page numeration)