Transmission coefficient and the reflection coefficient

Click For Summary
SUMMARY

The discussion focuses on the calculation of the transmission coefficient (T) and reflection coefficient for a particle transitioning from a higher potential to a lower potential, specifically when the particle is approaching a potential barrier. The derived formula for the transmission coefficient is T = 4a/(1+a)^2, where 'a' is the ratio of the final wave number to the initial wave number. The analysis concludes that T is solely dependent on the ratio of the wavelengths and does not differentiate between the size of the wavelengths or the nature of the object, whether it be a particle or a macroscopic object. The implications of the results suggest that for very high potential barriers, the likelihood of reflection increases significantly.

PREREQUISITES
  • Quantum mechanics fundamentals, particularly wave-particle duality
  • Understanding of potential barriers and tunneling phenomena
  • Familiarity with wave numbers and their relationship to wavelength
  • Basic calculus for graphing functions and analyzing turning points
NEXT STEPS
  • Study the derivation of the transmission and reflection coefficients in quantum mechanics
  • Learn about potential barriers in quantum tunneling scenarios
  • Explore the implications of wave-particle duality on macroscopic objects
  • Investigate the mathematical properties of the function T = 4a/(1+a)^2 and its graphical representation
USEFUL FOR

Students and professionals in physics, particularly those specializing in quantum mechanics, wave mechanics, and anyone interested in the behavior of particles at potential barriers.

jby
I tried to work out the transmission coefficient and
the reflection coefficient for a case similar to the
one referred by this website:
http://www.chembio.uoguelph.ca/educmat/chm386/rudiment/models/barrier/barsola.htm

but instead this time, I reverse the situation and
now, that particle I is heading from the right, ie
from a higher potential and a possibility that it will
be transmitted to the left, ie to a lower potential,
still with the same E > V.

I've drawn a diagram of the situation which I am
considering in my question using my own notations.
(As this is a bmp file, it may take some time to
load.)

http://www.geocities.com/ace_on_mark9909/reflection.htm


My confusion is regarding to the reflection and its
coefficient, which I've worked in steps here:

I state here the situation I am referring to: Supposing
the particle initially is at the potential V = 0,
heading to the left. At x = 0, there is the sudden
change in the potential to V = -V'.

Using p as the wave number, ie (2pi/lambda) for the
particle when at V = 0, and q as wave number for
particle at V = -V', I obtained the transmission
coefficient, T as 4pq/(p+q)^2.

By the condition of the potential 0 > -V', thus, p <
q, ie the wavelength at V = 0 > wavelength at V = -V'.


Let, q = ap, ie a = ratio of final wavenumber to
initial wave number: q/p. Since, q > p => a > 1.

We simplify the transmission coefficient to from
T = 4pq/(p+q)^2
to
T = 4a/(1+a)^2 ... (1)

From equation 1, it states that T is only dependent on
the ratio of the two wave number and hence dependent
only on the ratio of both wavelengths, and not on any
of the wavelength alone

=> the coefficient T does not discriminate on the size
on any of the wavelength alone but the ratio of the
magnitude of its wavelengths.

=> T does not distinguish between a particle or a
macroscopic object, eg, a ball.

From T = 4a/(1+a)^2, I've drawn a graph of it for a in
the range 0 <= a <= +infinity. I've uploaded to this
website:

http://www.geocities.com/ace_on_mark9909/transmission.htm


From the graph, it looks like there is a turning point
at a = 1, corresponding to T = 1, and slowly goes to
zero, as a -> infinity

By a -> infinity, we can say that the potential height
-V' approaches -infinity.

But, if the potential at x = 0, changes so sharply as
in approaching infinity, the graph shows T = 0, then,
it means that if I were to replace a particle with a
ball/human and is to approach this potential it is
almost likely to be reflected back...

Is there anything wrong with my maths? If not, how do
you interpret this result?
 
Last edited by a moderator:
Science news on Phys.org
This thread got no love in the Homework forum, so I'm kicking it here to Physics.
 
The energy of a macroscopic object is going to be so great that the potential isn't going to matter and your going to get complete transmission.

JMD

You should rework the solution, beacuse I doubt you get any reflection, but I haven't worked this out for a few years and can't remember right of the top of my head.
 
Last edited:

Similar threads

  • · Replies 10 ·
Replies
10
Views
3K
  • · Replies 14 ·
Replies
14
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 12 ·
Replies
12
Views
4K
  • · Replies 1 ·
Replies
1
Views
9K