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Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)
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Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Dec 16, 2015

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Page 1: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Department of Electronics

Nanoelectronics

05

Atsufumi Hirohata

12:00 Wednesday, 21/January/2015 (P/L 006)

Page 2: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Quick Review over the Last Lecture

Light quantum :

E = ( h )

( Compton ) scattering

Electron ( interference )

( De Broglie ) wave

Page 3: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Contents of Nanoelectonics

I. Introduction to Nanoelectronics (01) 01 Micro- or nano-electronics ?

II. Electromagnetism (02 & 03) 02 Maxwell equations 03 Scalar and vector potentials

III. Basics of quantum mechanics (04 ~ 06) 04 History of quantum mechanics 1 05 History of quantum mechanics 2 06 Schrödinger equation

IV. Applications of quantum mechanics (07, 10, 11, 13 & 14)

V. Nanodevices (08, 09, 12, 15 ~ 18)

Page 4: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

05 History of Quantum Mechanics 2

• Rutherford’s model

• Bohr’s model

• Balmer series

• Uncertainty principle

Page 5: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Early Models of an Atom

In 1904, J. J. Thomson proposed a plum pudding model :

Negatively charged “plums” (electrons) are surrounded by

positively charged “pudding.”

* http://www.wikipedia.org/** http://www.nararika.com/butsuri/kagakushi/genshi/genshiron.htm

In 1904, Hantaro Nagaoka proposed a Saturn model :

Negatively charged electrons rotate around positively-charged core.

Page 6: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Rutherford's Model

In 1909, Ernest Rutherford carried out a Au foil experiment :

-ray was introduced onto a very thin Au foil.

* http://www.wikipedia.org/

cannot be explained by the plum pudding model,

and the Saturn model was adopted.

Rutherford back scattering was observed.

The size of the core is estimated to be

10 -14 m.

Page 7: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Rutherford Back Scattering

Powerful tool for materials analysis :

* http://www.toray-research.co.jp/kinougenri/hyoumen/hyo_006.html

Analyser

Sample atoms

Example

Page 8: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Limitation of Rutherford's Model

In classical electromagnetism,

An electron rotating around the core loses its energy

by irradiating electromagnetic wave,

and falls into the positively-charged core.

In 1913, Niels H. D. Bohr proposed a quantum rule :

An electron can permanently rotate around the core

when occupying an orbital with

me : electron mass, v : electron speed, r : orbital radius,

n : quantum number and h : Planck constant

stable state

energy levels (n = 1, 2, 3, …)

* http://www.wikipedia.org/

Page 9: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Bohr's Model

Allowed transitions between the energy levels :

From the energy level of En to that of En’,

a photon is absorbed when En’ - En > 0.

a photon is released when En’ - En’ < 0.

* http://www.wikipedia.org/

Meaning of the quantum rule :

De Broglie wave length is defined as

By substituting this relationship into the quantum rule,

Electron as a standing wave in an orbital.

Page 10: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Proof of Bohr's Model

In 1914, James Franck and Gustav L. Hertz proved discrete energy levels :

An acceleration voltage is tuned to allow

diluted gas to absorb the energy.

* http://nobelprize.org/** http://www.wikipedia.org/

A proof of the quantum rule

Page 11: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Balmer Series in a Hydrogen Atom

In 1885, Johann Jakob Balmer proposed an empirical formula :

Balmer series observation :

Balmer formula :

* http://www.wikipedia.org/

: wavelength, B : constant (364.56 nm), n = 2 and

m : an integer (m > n)

A proof of the discrete electron orbitals

Page 12: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Rydberg Formula

In 1888, Johannes R. Rydberg generalised the Balmer formula :

Rydberg formula for Hydrogen :

Rydberg formula for atoms :

* http://www.wikipedia.org/

RH : Rydberg constant (10973731.57 m−1)

vac : wavelength of the light emitted in a vacuum,Z : atomic number, m and n : integers

Page 13: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Balmer Series in a Hydrogen Atom

Other series were also found :

* http://www.bigs.de/en/shop/htm/termsch01.html

Lyman series(1906)

Ultra violet

Balmer series(1885)

Visible light

Brackett series(1922)

Near infrared

Paschen series(1908)Infrared

Pfund series(1924)

Far infrared

Humphreys series(1953)

Far infrared

Page 14: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Heisenberg's Thought Experiment

In 1927, Werner Karl Heisenberg proposed the uncertainty principle :

Resolution of a microscope is defined as

* http://www.wikipedia.org/

In order to minimise ,

Larger

Small

Here,

Small large p (damage to samples)

Also, larger difficult to identify paths

incident wave

x-direction electron

In addition, incident wave can be reflected within

Momentum along x is within

Page 15: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Observation of the Uncertainty Principle

Zero-point motion :

He does not freeze near 0 K under atmospheric pressure.

Spin fluctuation in an itinerant magnet :

* http://www.e-one.uec.ac.jp/~kuroki/cobalt.html

Page 16: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Precise Quantum Physical Definition

Relationship between an observation error in position and disturbance in momentum :

Heisenberg’s uncertainty principle using operators :

Heisenberg’s uncertainty principle using standard deviations :

Here, communication relation :

If A and B are commutative operators, the right-hand side is 0. This leads the error and disturbance to be 0.

However, A and B are not commutative operators, the right-hand side is not 0. This leads the error and disturbance to have a trade-off.

→ Precise definition

Page 17: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Corrections to Heisenberg’s Uncertainty Principle

Ozawa’s relationship : *

Optical proof : **

* M. Ozawa, Phys. Rev. A 67, 042105 (2003);** S.-Y. Baek et al., Sci. Rep. 3, 2221 (2013).

Page 18: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Experimental Data

Error and disturbance measured :

** S.-Y. Baek et al., Sci. Rep. 3, 2221 (2013).

Page 19: Department of Electronics Nanoelectronics 05 Atsufumi Hirohata 12:00 Wednesday, 21/January/2015 (P/L 006)

Ozawa’s Relationship

Ozawa’s relationship :

** S.-Y. Baek et al., Sci. Rep. 3, 2221 (2013).