When the mean free path of the electron is longer than the dimension of the medium through which the electron travels is called Ballistic transport
BALLISTIC
TRANSPORT
When
the length 'L' of the conductor becomes much smaller than the mean free path
'L' the transport is termed 'ballistic' meaning that the electrons do not
scatter during the time it takes to travel through the conductor.
For
example, ballistic transport can be observed in a metal nano wire. This is
because the wire is of the size of a nanometer and the mean free path can be
longer than in a metal.
The
mean free path [The average distance that the electron can travel freely] can
be increased by reducing the number of impurities in a crystal or by lowering
its temperature.
Ballistic transport conditions are
(i) L << Lm and
(ii) L << Lϕ
Where
L
→ Length of the conductor
Lm
→ mean free path [length that the electron can travel before having an elastic
collision]
Lϕ → Length over which an
electron can travel before having an inelastic collision. This is also called
the phase-coherence length, since it is the length over which an electron wave
function retains its coherence.
For
L << Lm and L << L
ϕ we have ballistic transport.
Ballistic
transport occurs over very small length scales, and is obviously coherent.
The
electron doesn't hit anything as it travels through the material, and,
therefore, there is no momentum or phase relaxation. Thus, in Ballistic
material, the electron's wave function can be obtained from schrodinger's
equation.
One
practical application of ballistic transport is to ultra-short-channel
semiconducting FETS or carbon nano tube transistors.
Physics for Information Science: Unit V: Nanodevices and Quantum Computing : Tag: : Definition, Explanation, Condition, Application - Ballistic Transport
Physics for Information Science
PH3256 2nd Semester CSE Dept | 2021 Regulation | 2nd Semester CSE Dept 2021 Regulation
Professional English II
HS3251 2nd Semester 2021 Regulation | 2nd Semester Common to all Dept 2021 Regulation
Statistics and Numerical Methods
MA3251 2nd Semester 2021 Regulation M2 Engineering Mathematics 2 | 2nd Semester Common to all Dept 2021 Regulation
Engineering Graphics
GE3251 eg 2nd semester | 2021 Regulation | 2nd Semester Common to all Dept 2021 Regulation
Physics for Electrical Engineering
PH3202 2nd Semester 2021 Regulation | 2nd Semester EEE Dept 2021 Regulation
Basic Civil and Mechanical Engineering
BE3255 2nd Semester 2021 Regulation | 2nd Semester EEE Dept 2021 Regulation
Electric Circuit Analysis
EE3251 2nd Semester 2021 Regulation | 2nd Semester EEE Dept 2021 Regulation
Physics for Electronics Engineering
PH3254 - Physics II - 2nd Semester - ECE Department - 2021 Regulation | 2nd Semester ECE Dept 2021 Regulation
Electrical and Instrumentation Engineering
BE3254 - 2nd Semester - ECE Dept - 2021 Regulation | 2nd Semester ECE Dept 2021 Regulation
Circuit Analysis
EC3251 - 2nd Semester - ECE Dept - 2021 Regulation | 2nd Semester ECE Dept 2021 Regulation
Materials Science
PH3251 2nd semester Mechanical Dept | 2021 Regulation | 2nd Semester Mechanical Dept 2021 Regulation
Basic Electrical and Electronics Engineering
BE3251 2nd semester Mechanical Dept | 2021 Regulation | 2nd Semester Mechanical Dept 2021 Regulation
Physics for Civil Engineering
PH3201 2021 Regulation | 2nd Semester Civil Dept 2021 Regulation
Basic Electrical, Electronics and Instrumentation Engineering
BE3252 2021 Regulation | 2nd Semester Civil Dept 2021 Regulation
Physics for Information Science
PH3256 2nd Semester CSE Dept | 2021 Regulation | 2nd Semester CSE Dept 2021 Regulation
Basic Electrical and Electronics Engineering
BE3251 2nd Semester CSE Dept 2021 | Regulation | 2nd Semester CSE Dept 2021 Regulation
Programming in C
CS3251 2nd Semester CSE Dept 2021 | Regulation | 2nd Semester CSE Dept 2021 Regulation