Question 705033

SCQHARD

An integral is given by dxdyexp[(x2+y2+2axy)]\int_{-\infty}^{\infty} dx \int_{-\infty}^{\infty} dy \exp[-(x^2 + y^2 + 2axy)], where aa is a real parameter. The full range of values of aa for which the integral is finite, is

(A)

<a<-\infty < a < \infty

(B)

2<a<2-2 < a < 2

(C)

1<a<1-1 < a < 1

(D)

1a1-1 \le a \le 1

Detailed Solution

We are given the integral:

I=exp[(x2+y2+2axy)]dxdyI = \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} \exp[-(x^2 + y^2 + 2axy)] dx dy

We need to eliminate the coupled term (2axy)(2axy) from the exponent. For this, we use a standard linear transformation that rotates the axes by 4545^\circ:

Step 1: Define the Transformation Let the new variables be uu and vv, where:

x=u+v2x = \frac{u + v}{\sqrt{2}}

y=uv2y = \frac{u - v}{\sqrt{2}}

Step 2: Calculate the Jacobian Now, we differentiate xx and yy with respect to uu and vv to form the Jacobian matrix:

J=det(12121212)J = \det \begin{pmatrix} \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \\ \frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} \end{pmatrix}

Solving the determinant:

J=(12×12)(12×12)=1212=1J = \left(\frac{1}{\sqrt{2}} \times -\frac{1}{\sqrt{2}}\right) - \left(\frac{1}{\sqrt{2}} \times \frac{1}{\sqrt{2}}\right) = -\frac{1}{2} - \frac{1}{2} = -1

The area scale factor is always positive, so we take its absolute value:

J=1=1|J| = |-1| = 1

This means in the new coordinate system, dxdy=dudvdx dy = du dv. (Since this is a pure rotation, the area neither stretches nor shrinks).

Step 3: Convert the Exponent to the New Variables Now, substitute the transformation formulas into the original exponent x2+y2+2axyx^2 + y^2 + 2axy:

First, let's evaluate x2+y2x^2 + y^2:

x2+y2=(u+v2)2+(uv2)2=u2+v2+2uv+u2+v22uv2=u2+v2x^2 + y^2 = \left(\frac{u + v}{\sqrt{2}}\right)^2 + \left(\frac{u - v}{\sqrt{2}}\right)^2 = \frac{u^2 + v^2 + 2uv + u^2 + v^2 - 2uv}{2} = u^2 + v^2

Next, evaluate 2xy2xy:

2xy=2(u+v2)(uv2)=2(u2v22)=u2v22xy = 2 \left(\frac{u + v}{\sqrt{2}}\right) \left(\frac{u - v}{\sqrt{2}}\right) = 2 \left(\frac{u^2 - v^2}{2}\right) = u^2 - v^2

Substituting these back into the exponent:

(u2+v2)+a(u2v2)(u^2 + v^2) + a(u^2 - v^2)

u2(1+a)+v2(1a)u^2(1 + a) + v^2(1 - a)

Notice that the cross-term (coupled term) has completely vanished!

Step 4: Evaluate the Integral and Check Convergence Conditions The limits of integration remain from -\infty to \infty. The new integral becomes:

I=exp[u2(1+a)v2(1a)]dudvI = \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} \exp[-u^2(1 + a) - v^2(1 - a)] du dv

Since uu and vv are now independent, we can split the integral into two separate standard 1D Gaussian integrals:

I=(exp[u2(1+a)]du)×(exp[v2(1a)]dv)I = \left( \int_{-\infty}^{\infty} \exp[-u^2(1 + a)] du \right) \times \left( \int_{-\infty}^{\infty} \exp[-v^2(1 - a)] dv \right)

A standard Gaussian integral exp(αz2)dz\int \exp(-\alpha z^2) dz is finite (convergent) only if the constant α>0\alpha > 0.

Therefore, we obtain two conditions for the two integrals:

  1. For the first integral: 1+a>0    a>11 + a > 0 \implies a > -1
  2. For the second integral: 1a>0    a<11 - a > 0 \implies a < 1

Both conditions are simultaneously satisfied only when the value of aa lies between 1-1 and 11.

Final Answer: The full range of values of aa for which the integral is finite is 1<a<1-1 < a < 1.

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