Microsoft Word - Maser
Donor type semiconductor at low temperature
as maser active medium
Yuri Kornyushin
Maître Jean Brunschvig Research Unit, Chalet Shalva, Randogne, CH-3975
In some semiconductors donor impurity atoms can attract additional
electrons, forming negative donor impurity ions. Thus we have 3 energy
levels for electrons: zero energy levels at the bottom of the conductivity
band, negative energy levels of the bounded electrons of the negative
donor impurity ions, and deeper negative energy levels of the outer
electrons of the neutral donor impurity atoms. So the donor impurity
atoms could serve as active centres for a maser. The maximum achievable
relative population is 0.5. Typical wavelength of the generated oscillation
is 0.14 mm; three level scheme could be realized at rather low
temperatures, considerably lower than 6 K.
Let us consider some donor impurity atom in a donor-type semiconductor having
one more outer electron than the host atom of a semiconductor (e.g., the host silicon
atom). In the simplest case of a non-degenerate standard conductivity band the
equation of a motion of a superfluous electron is the same as that for the electron in a
hydrogen atom [1]. The bond energy at that is as follows [1]:
Ebd = (m0e
)(m/m0
), (1)
where m0 is the free electron mass, m is the effective electron mass in semiconductor
conductivity band, e is the electron charge, and  is the Planck constant divided by 2.
Comparative to the bond energy in a hydrogen atom (see, e.g., [2]) the right-hand
part of Eq. (1) contains additional factor (m/m0
). At m = 0.1m0 and  = 12 [1] this
factor, (m/m0
) = 6.94410
Hydrogen atom can attract an additional electron, forming negative hydrogen ion
[3]. The electron affinity of a free electron to a hydrogen atom is Eah = 0.754 eV [3].
The bond energy in a hydrogen atom, Ebh = (m0e
) = 13.598 eV [3]. Taking into
account that in a donor semiconductor we have an additional factor (m/m0
), we have
the affinity of a conductivity band electron to a donor impurity atom Ead =
0.754(m/m0
) eV and Ebd = 13.598(m/m0
) eV. At m = 0.1m0 and  = 12 [1] we have
Ead = 5.23610
eV = 6.076 K and Ebd = 9.44310
So at temperature considerably lower than Ead (about 6 K here) we have donor
atoms acting as active maser centres. We have three energy levels of electrons: zero
energy levels at the bottom of the conductivity band, negative energy levels of
electron, forming negatively charged donor ions, and deeper negative energy levels of
the outer electron of the neutral donor impurity atoms. So we can pump some outer
electrons of some neutral donor impurity atoms to the conductivity band. At low
enough temperature these electrons will form negative impurity ions with some other
neutral donor impurity atoms, thus forming highly populated levels above the ground
state level, Ebd. When high population of the upper levels is achieved, the frequency,
Ebd  Ead = 8.9210
eV = 2.1410
(1/s) = 0.14 mm, could be generated or
amplified. It is rather obvious that the maximum concentration of the negative donor
impurity ions, which could be achieved, is 0.5nd (nd is the number of the donor
impurity atoms per unit volume of a semiconductor).
References
1. A. L. Efros. Semiconductors, in: Encyclopaedic Dictionary Solid State Physics, V.
2 (Kiev: Naukova Dumka, 1998), p. 91 (in Russian).
2. L. D. Landau and E. M. Lifshits, Quantum Mechanics (Oxford: Pergamon, 1986).
3. 1988 CRC Handbook of Chemistry and Physics, ed. R. C. Weast (Boca Raton, FL:
CRC).

  In some semiconductors donor impurity atoms can attract additional electrons,
forming negative donor impurity ions. Thus we have 3 energy levels for
electrons: zero energy levels at the bottom of the conductivity band, negative
energy levels of the bounded electrons of the negative donor impurity ions, and
deeper negative energy levels of the outer electrons of the neutral donor
impurity atoms. So the donor impurity atoms could serve as active centres for a
maser. The maximum achievable relative population is 0.5. Typical wavelength of
the generated oscillation is 0.14 mm; three level scheme could be realized at
rather low temperatures, considerably lower than 6 K.

Microsoft Word - Maser
Donor type semiconductor at low temperature
as maser active medium
Yuri Kornyushin
Maître Jean Brunschvig Research Unit, Chalet Shalva, Randogne, CH-3975
In some semiconductors donor impurity atoms can attract additional
electrons, forming negative donor impurity ions. Thus we have 3 energy
levels for electrons: zero energy levels at the bottom of the conductivity
band, negative energy levels of the bounded electrons of the negative
donor impurity ions, and deeper negative energy levels of the outer
electrons of the neutral donor impurity atoms. So the donor impurity
atoms could serve as active centres for a maser. The maximum achievable
relative population is 0.5. Typical wavelength of the generated oscillation
is 0.14 mm; three level scheme could be realized at rather low
temperatures, considerably lower than 6 K.
Let us consider some donor impurity atom in a donor-type semiconductor having
one more outer electron than the host atom of a semiconductor (e.g., the host silicon
atom). In the simplest case of a non-degenerate standard conductivity band the
equation of a motion of a superfluous electron is the same as that for the electron in a
hydrogen atom [1]. The bond energy at that is as follows [1]:
Ebd = (m0e
)(m/m0
), (1)
where m0 is the free electron mass, m is the effective electron mass in semiconductor
conductivity band, e is the electron charge, and  is the Planck constant divided by 2.
Comparative to the bond energy in a hydrogen atom (see, e.g., [2]) the right-hand
part of Eq. (1) contains additional factor (m/m0
). At m = 0.1m0 and  = 12 [1] this
factor, (m/m0
) = 6.94410
Hydrogen atom can attract an additional electron, forming negative hydrogen ion
[3]. The electron affinity of a free electron to a hydrogen atom is Eah = 0.754 eV [3].
The bond energy in a hydrogen atom, Ebh = (m0e
) = 13.598 eV [3]. Taking into
account that in a donor semiconductor we have an additional factor (m/m0
), we have
the affinity of a conductivity band electron to a donor impurity atom Ead =
0.754(m/m0
) eV and Ebd = 13.598(m/m0
) eV. At m = 0.1m0 and  = 12 [1] we have
Ead = 5.23610
eV = 6.076 K and Ebd = 9.44310
So at temperature considerably lower than Ead (about 6 K here) we have donor
atoms acting as active maser centres. We have three energy levels of electrons: zero
energy levels at the bottom of the conductivity band, negative energy levels of
electron, forming negatively charged donor ions, and deeper negative energy levels of
the outer electron of the neutral donor impurity atoms. So we can pump some outer
electrons of some neutral donor impurity atoms to the conductivity band. At low
enough temperature these electrons will form negative impurity ions with some other
neutral donor impurity atoms, thus forming highly populated levels above the ground
state level, Ebd. When high population of the upper levels is achieved, the frequency,
Ebd  Ead = 8.9210
eV = 2.1410
(1/s) = 0.14 mm, could be generated or
amplified. It is rather obvious that the maximum concentration of the negative donor
impurity ions, which could be achieved, is 0.5nd (nd is the number of the donor
impurity atoms per unit volume of a semiconductor).
References
1. A. L. Efros. Semiconductors, in: Encyclopaedic Dictionary Solid State Physics, V.
2 (Kiev: Naukova Dumka, 1998), p. 91 (in Russian).
2. L. D. Landau and E. M. Lifshits, Quantum Mechanics (Oxford: Pergamon, 1986).
3. 1988 CRC Handbook of Chemistry and Physics, ed. R. C. Weast (Boca Raton, FL:
CRC).
