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REQUIREMENTS FOR AN ACCEPTABLE (WELL-BEHAVED) WAVEFUNCTION 
 
1. The wave function ? must be continuous.  All its partial derivatives must also be 
continuous (partial derivatives are etc. 
y
 , 
?
?
?
? ? ?
x
).  This makes the wave function 
“smooth”. 
 
2. The wave function ? must be quadratically integrable.  This means that the integral 
t ? ? d  
*
must exist. 
?
 
3. Since  is the probability density, it must be single valued. 
?
t ? ? d  
*
4. The wave functions must form an orthonormal set.  This means that  
• the wave functions must be normalized.  
 
?
8
8 _
*
  t ? ? d
i i
 = 1 
• the wave functions must be orthogonal. 
 
?
8
8 _
*
  t ? ? d
j i
 = 0 
OR         =   d
ij
  where d
ij
   = 1 when i = j and  d
ij
  = 0 when i ? j 
?
8
8 _
*
  t ? ? d
j i
 
d
ij
  is called Kronecker delta 
 
5. The wave function must be finite everywhere. 
 
6. The wave function must satisfy the boundary conditions of the quantum mechanical 
system it represents.  
 
Page 2


REQUIREMENTS FOR AN ACCEPTABLE (WELL-BEHAVED) WAVEFUNCTION 
 
1. The wave function ? must be continuous.  All its partial derivatives must also be 
continuous (partial derivatives are etc. 
y
 , 
?
?
?
? ? ?
x
).  This makes the wave function 
“smooth”. 
 
2. The wave function ? must be quadratically integrable.  This means that the integral 
t ? ? d  
*
must exist. 
?
 
3. Since  is the probability density, it must be single valued. 
?
t ? ? d  
*
4. The wave functions must form an orthonormal set.  This means that  
• the wave functions must be normalized.  
 
?
8
8 _
*
  t ? ? d
i i
 = 1 
• the wave functions must be orthogonal. 
 
?
8
8 _
*
  t ? ? d
j i
 = 0 
OR         =   d
ij
  where d
ij
   = 1 when i = j and  d
ij
  = 0 when i ? j 
?
8
8 _
*
  t ? ? d
j i
 
d
ij
  is called Kronecker delta 
 
5. The wave function must be finite everywhere. 
 
6. The wave function must satisfy the boundary conditions of the quantum mechanical 
system it represents.  
 
POSTULATES OF QUANTUM MECHANICS 
 
1. The state of a quantum-mechanical system is completely specified by its wave function 
?(r).  ?
*
(r) ?(r) dxdydz is the probability that the particle lies in the volume element 
dxdydz, located at r. (Note: we are considering the time independent wave function for all 
our work). 
 
2. To every observable in classical mechanics, there corresponds a linear operator in quantum 
mechanics. 
 
3. In any measurement of the observable associated with the operator
^
A , the only values that 
will ever be observed are the eigenvalues a, which satisfy the eigenvalue equation 
 
(r) a    (r) A
ˆ
? = ? 
 
4. If a system is in a state described by a normalized wave function ?, then the average value 
(or the expectation value) of the observable corresponding to operator A is given by  
 
t d  A
ˆ
     
*
? ? = > <
?
8
8 -
a 
 
 
5. The wave function of a system evolves in time according to the time dependent 
Schrodinger equation 
 
dt
d
  i     t) (x, H
ˆ
?
= ? h 
 
 
 
 
 
 
 
 
 
 
 
 
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FAQs on Requirements for a well behaved wave function - AP Physics 2 - Grade 9

1. What are the requirements for a well-behaved wave function?
Ans. A well-behaved wave function must satisfy several criteria. Firstly, it should be single-valued, meaning it should have a unique value at each point in space. Secondly, it should be continuous, without any abrupt changes or discontinuities. Additionally, the wave function must be square-integrable, meaning its absolute value squared integrated over all space should be finite. Lastly, the wave function should also be differentiable, allowing for the calculation of derivatives.
2. Why is it important for a wave function to be single-valued?
Ans. A single-valued wave function is important because it ensures that there is a unique probability associated with each point in space. If the wave function were not single-valued, it would lead to inconsistencies in the predictions of quantum mechanics. By having a unique value at each point, the wave function allows us to calculate the probability density and make meaningful predictions about the behavior of quantum systems.
3. What does it mean for a wave function to be square-integrable?
Ans. Square-integrability is a requirement for a well-behaved wave function, meaning that the absolute value squared of the wave function integrated over all space should be finite. This condition ensures that the total probability of finding a particle in any region of space is well-defined and finite. If a wave function is not square-integrable, it implies that the particle's probability of being found somewhere in space is either infinite or undefined, which is not physically meaningful.
4. Why is it necessary for a wave function to be continuous?
Ans. Continuity of the wave function is important because abrupt changes or discontinuities in the wave function would result in infinite or undefined values for certain physical quantities such as momentum or energy. This would lead to nonsensical predictions in quantum mechanics. By requiring continuity, we ensure that the wave function smoothly describes the behavior of a quantum system, allowing for meaningful calculations and predictions.
5. Can a wave function be non-differentiable?
Ans. No, a well-behaved wave function must be differentiable. Differentiability of the wave function is necessary for the calculation of derivatives, which are used to determine various physical quantities such as momentum and energy. If a wave function were non-differentiable at certain points, it would result in undefined or infinite values for these quantities, leading to inconsistencies in quantum mechanics. Therefore, a differentiable wave function is a fundamental requirement for a meaningful description of quantum systems.
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