/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q1P (a) Show that the set of all squ... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

(a) Show that the set of all square-integrable functions is a vector space (refer to Section A.1 for the definition). Hint: The main problem is to show that the sum of two square-integrable functions is itself square-integrable. Use Equation 3.7. Is the set of all normalized functions a vector space?

(b) Show that the integral in Equation 3.6satisfies the conditions for an inner product (Section A.2).

Short Answer

Expert verified

a) Two square-integrable functions add up to a square-integrable function.

b) The integral in equation 3.6 satisfies the conditions for an inner product.

Step by step solution

01

Concept used

Equation 3.7 follows Schwarz inequality:

∫abfx*gxdx≤∫abfx2dx∫abgx2dx

Equation 3.6 define the inner product of two functions

fIg=∫abfx*gxdx

02

Given information from question

a)

Let fxand gxbe square-integrable, then we need to prove thathx=fx+gxis also square-integrable,

h2=f+g*f+g=f2+g2+f*g+g*f

The integration is,

∫h2dx=∫f2dx+∫g2dx+∫f*gdx+∫f*gdx*

since both fxandgxare square-integrable, then the first two terms are finite, using Schwarz inequality, we can write the third and the fourth integrals in terms of the first and the second integral:

∫abfx*gxdx≤∫abfx2dx∫abgx2dx

Therefore, the last two integrals are finite too. Hence ∫h2dxis finite, therefore Two square-integrable functions add up to a square-integrable function. Now let ψxbe a vector with a value or component for every value of x . If a set of vectors meets two criteria, it can be called a vector space:

- If a vector ψ1xis in the set, then so is Aψxfor any complex scalar A

- If two vectors ψ1xand ψ2xare in the set, then so is their sum ψ1x+ψ2x

these two conditions can be combined by saying that if two vectors ψ1xand ψ2xare in the set, then so is their linear combination Aψ1x+Bψ2x , for any complex scalars and AWe can see from this definition that the above-mentioned collection of all normalizable functions is not a vector space. For example, if 1 is true for a vectorψx , then it is not true if we multiply ψxby any scalar Awhere A≠1.

03

The definition of an inner product of two vectors

b)

The definition of an inner product of two vectors requires that it satisfies three conditions:

→g\f=f\g*→f\f≥0andf\f=0ifandonlyif\f>=0→h\(A\f+B\g>)=Ah\f+Bh\g

the first condition is trivial to prove, as:

g\f=∫abgx*fxdx=∫abfx*gxdx*=f\g*

For the second condition, we can use:

f\f=∫-∞∞f*xfxdx

To prove that f\f≥0and f\f=0if and only if \f>=0. For the third condition, we have:

h\A\f>+B\g)=∫-∞∞h*xAfx+h*xBgxdx=∫-∞∞h*xAfxdx+∫-∞∞h*xBgxdx=A∫-∞∞h*xfxdx+B∫-∞∞h*xgxdx=Ah\f+Bh\g

therefore, Equation 3.6's integral satisfies the requirements for an inner product.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Find the momentum-space wave function, Φ(p,t),for a particle in the ground state of the harmonic oscillator. What is the probability (to 2significant digits) that a measurement of p on a particle in this state would yield a value outside the classical range (for the same energy)? Hint: Look in a math table under "Normal Distribution" or "Error Function" for the numerical part-or use Mathematica.

The Hermitian conjugate (or adjoint) of an operator Q^is the operatorQ^†such that

⟨f∣Q^g⟩=⟨Q^†f∣g⟩ (´Ú´Ç°ù²¹±ô±ôfandg).

(A Hermitian operator, then, is equal to its Hermitian conjugate:Q^=Q^†)

(a)Find the Hermitian conjugates of x, i, andd/dx.

(b) Construct the Hermitian conjugate of the harmonic oscillator raising operator,a+(Equation 2.47).

(c) Show that(Q^R^)†=R^†Q^†.

Consider a three-dimensional vector space spanned by an Orthonormal basis 1>,2>,3>. Kets α>and β>are given by

|α⟩=i|1⟩-2|2⟩-i|3⟩,   |β>=i|1⟩+2|3⟩.

(a)Construct<αand <β(in terms of the dual basis

⟨1|,⟨2|,⟨3|).
(b) Find ⟨α∣β⟩and⟨β∣α⟩,and confirm that

⟨β∣α⟩=⟨α∣β⟩*.
(c)Find all nine matrix elements of the operatorAÁåœâ‰¡|α⟩⟨β|, in this basis, and construct the matrix A. Is it hermitian?

Extended uncertainty principle.The generalized uncertainty principle (Equation 3.62) states that

σA2σB2≥14<C>2

whereC^≡-i[A^,B^̂]..

(a) Show that it can be strengthened to read

σA2σB2≥14(<C>2+<D>2) [3.99]

whereD^≡A^B^+B^A^-2⟨A⟩⟨B⟩.. Hint: Keep the term in Equation 3.60

(b) Check equation 3.99 for the caseB=A(the standard uncertainty principle is trivial, in this case, sinceC^=0; unfortunately, the extended uncertainty principle doesn't help much either).

(a) Check that the eigenvalues of the hermitian operator in Example 3.1 are real. Show that the eigenfunctions (for distinct eigenvalues) are orthogonal.

(b) Do the same for the operator in Problem 3.6.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.