Bohr Model applied to Excitons

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Homework Help Overview

The discussion revolves around the application of the Bohr model to excitons in semiconductors, specifically silicon. Participants are exploring the properties of excitons, which are described as bound electron-hole pairs, and are comparing them to hydrogen-like atoms. The problem includes estimating the radius and ground state energy of an exciton, as well as examining the separation between silicon atoms and the relationship between exciton binding energy and thermal energy.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the calculation of the exciton radius and energy, with some questioning the effective mass used in the calculations. There are inquiries about how to determine the separation between silicon atoms and the relevance of this distance to the exciton radius. Additionally, participants are examining the comparison between exciton binding energy and average kinetic energy in silicon.

Discussion Status

The discussion is ongoing, with participants providing various insights and calculations. Some have offered guidance on how to approach the problem, while others are exploring different interpretations of the parameters involved. There is no explicit consensus yet, as participants are still clarifying concepts and calculations.

Contextual Notes

Participants note the use of specific constants and values relevant to silicon, such as the permittivity and effective masses. There is also mention of the need to consider gravitational potential energy in the context of electrostatic interactions, with some suggesting it may be negligible.

adamaero
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An exciton is a bound electron-hole pair (in a semiconductor). For this problem, think of an exciton as a hydrogen-like atom, with a negatively charged electron and positively charged hole orbiting each other.

The permittivity of free space (ε0) is replaced with permittivity of the semiconductor (ε = 12).
The mass of the electron is replaced with the effective mass of the electron-hole pair.

1. Homework Statement (bold below is what I really need help on)

A) Estimate the radius in nm and the ground state energy in eV for an exciton in Si.

B) Approximately how large is the separation between atoms in a crystal of silicon? How does the radius compare with this number?

C) Silicon atoms have an average kinetic energy of T*kB. How does the exciton binding energy (E1) compare with this number? What does this mean?

D) All this is about electrostatic potential energy. Prove that it's reasonable to neglect the gravitational potential energy.

me = 9.1*10-31
eV = 1.602×10−19 J (N*m)
h = 6.626*10-34
ħ = 1.055*10-34
a0 = 0.0529 nm
ε*ε0 = 1.0359*10-10

permittivity of silicon = εSi = kSiε0 where k = dielectric constant

effective masses
me* = 0.26me
mh* = 0.36me

Homework Equations


r = mek2e4/(πħ3)

me*mh*/(me* + mh*) = 0.15me

r = n2h2*1.0359*10-10/(z*π*meffectivee2)

The Attempt at a Solution


A)
upload_2016-10-22_10-2-33.png


12*a0/0.15 = 4.2nm (n2/z)

upload_2016-10-22_10-3-17.png


Ry = -13.6eV

B) I do not remember chemistry much. How is the separation between silicon atoms found?

C) 300*1.38*10-23 m2kg/s2 = 4.14*10-23
E1 = ?

D) PEelectrostatic = kqQ/r
images.slideplayer.com/22/6421287/slides/slide_3.jpg
FE = qE
Fg = mg
∴ qE = mg
& as long as qE/m is much larger than g, gravity can be ignored.

Sources
http://www.course-notes.org/book/export/html/10891
https://upload.wikimedia.org/wikipedia/commons/9/97/Exciton_energy_levels.jpg
 
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adamaero said:
Ry = -13.6eV
You get the same Rydberg constant as for hydrogen?

adamaero said:
B) I do not remember chemistry much. How is the separation between silicon atoms found?
Google :smile: There is no way to find that by first principles, so just Google "silicon interatomic distance".

adamaero said:
C) 300*1.38*10-23 m2kg/s2 = 4.14*10-23
E1 = ?
That should be the binding energy. Do you remember how to find that for hydrogen?
 
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Oh yes, sorry, with ε:
The energy (for part A) is mee4/[8(h*1.0359*10-10)2]
= (9.1*10^-31)(e^4)/[8*((6.626*10^-34)*(1.0359*10^-10))^2]
= 1.32*1057
Was that suppose to be a different mass?

Thank you. I did Google it. Although, I either searched the wrong phrase or thought it wasn't simple from the results that came up earlier.
atomic radius = 0.132 nm
lattice parameter = 0.543 nm
nearest neighbor distance = 0.235 nm
Looks like the calculation before (4.2 nm) is wrong?

The binding energy of an electron to the nucleus in the hydrogen atom is 13.6 eV.
So the binding energy is the absolute value of Rydberg energy??
 
BE=(mp+me-mH)*c2
BE = (938MeV/c2 + 0.511MeV/c2 - 938.3MeV/c2)*c2 =
(938.484+ 0.511 - 938.783)*10^6
= 212keV

938.783 MeV (mass of hydrogen)
1.673e-27 kg (mass of proton)
>> 1 eV = 1.602e-19 J <<
>> 1 J = m3 kg / s2 <<
[(1.673e-27)/(1.602e-19)]*c2
= 9.3989e8
= 939.89e6
= 939.89 MeV
 
sol.

A) The 4.2nm (n2/z) is correct. The energy is found this way: E = m*e4/(8h2ε2), but
B) 0.235 nm or 0.543 nm means that there are multiple atoms in-between each
C) This is the same E1, but can be modified from more general E1 = me4/(8h2ε02) = -13.6 eV... E = E1*(mT/m)/[(ε/ε0)2]
 

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