Anthony Kent -- SASER -- Sound Amplification by Stimulated
Emission of Radiation

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**Anthony KENT**

**SASER** **( Phonon Laser )**

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[**http://www.aip.org/pnu/2006/779.html**](http://www.aip.org/pnu/2006/779.html)  
American Institute of Physics   
***Physics News* ( Number 779 ); June 2, 2006**

**A New Kind of Acoustic Laser**

**by** **Phil Schewe**

**Sound amplification by stimulated emission of radiation**,
or **SASER**, is the acoustic analog of a laser. Instead of
a feedback-built potent wave of electromagnetic radiation, a
saser would deliver a potent ultrasound wave.

The concept has been around for years and several labs have
implemented models with differing features. In a new version,
undertaken by scientists from the University of Nottingham
(Anthony Kent, anthony.kent@nottingham.ac.uk) in the U.K. and
the Lashkarev Institute of Semiconductor Physics in Ukraine, the
gain medium -- that is, the medium where the amplification takes
place -- consists of stacks (or a superlattice) of thin layers
of semiconductors which together form "quantum wells."

In these wells, really just carefully confined planar regions,
electrons can be excited by parcels of ultrasound, which
typically possess millielectronvolts of energy, equivalent to a
frequency of 0.1-1 terahertz. And just as coherent light can
build up in a laser by the concerted, stimulated emission of
light from a lot of atoms, so in a saser coherent sound can
build up by the concerted emission of phonons from a lot of
quantum wells in the superlattice.

In lasers the light buildup is maintained by a reflective
optical cavity. In the U.K.-Ukraine saser, the acoustic buildup
is maintained by an artful spacing of the lattice layer
thicknesses in such a way that the layers act as an acoustic
mirror.

Eventually the sound wave emerges from the device at a narrow
angular range, as do laser pulses. The monoenergetic nature of
the acoustic emission, however, has not yet been fully probed.
The researchers believe their saser is the first to reach the
terahertz frequency range while using also modest electrical
power input. Terahertz coherent sound is itself a relatively new
field of research. Essentially ultrasound with wavelengths
measured in nanometers, terahertz acoustical devices might be
used in modulating light waves in optoelectronic devices.

**Kent *et* al., Physical Review Letter, 2 June 2006**
  
Contact :  Anthony Kent, anthony.kent@nottingham.ac.uk

http://aip.org/png/2006/260.htm

A schematic illustrating how the acoustic analog of a laser
works. The top image shows the structure of a superlattice of
semiconductor layers and confined acoustic waves undergoing
amplification. The bottom image shows the energy levels of
electrons confined in the superlattice layers; one phonon in can
produce two phonons coming out.

![](saser.jpg)

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**KR910002238**   
**SASER DIODE DRIVING CIRCUIT**

1991-04-08   
Inventor(s):  NAGANO GAZHI [JP]   
Applicant(s):  TOKYO SHIBAURA ELECTRIC CO [JP]   
Classification:  - international:  H01S3/00; H01S3/00;
(IPC1-7): H01S3/00

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**GB2343605**   
**Nonlinear Saser with Multiple Pumps**

2000-05-10   
CAHILL MARK DAVID   
Classification:  - international:  G10K15/04;
G10K15/04; (IPC1-7): G10K15/04; H04R23/00- European: 
G10K15/04

**Abstract** -- The amplification, detection or generation
of a sound 3 by causing it to form a standing wave, a sasing
mode, and causing this standing wave to interact with other
standing waves, pump modes, 1 of sound. At least one of the pump
modes has a frequency close to that of the sound to be
amplified, detected or generated, and another one has a
different frequency, the amplitudes of these other standing
waves varying in time or space.

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**GB2327026**   
**Non-Linear Saser**

1999-01-06   
Inventor(s):  CAHILL MARK DAVID   
Classification: - international:  G10K15/04; G10K15/04;
(IPC1-7): G10K11/08; H04R23/00 - European:  G10K15/04

**Abstract** --  A sound wave of a particular frequency
and travelling in a particular direction is amplified by causing
it to interact with a high-amplitude standing wave of the same
frequency, but oscillating in a different direction to the sound
wave. The standing wave (pump mode) is set up in a suitable
medium, e.g. a liquid alcohol such as ethanol, between acoustic
mirrors 1. The sound wave to be amplified (sasing mode) enters
the medium through partly-transparent mirrors 2.

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[**http://en.wikipedia.org/wiki/Sound\_Amplification\_by\_Stimulated\_Emission\_of\_Radiation**](http://en.wikipedia.org/wiki/Sound_Amplification_by_Stimulated_Emission_of_Radiation)

**SASER**

A SASER operates on principles remarkably similar to those of a
laser. A stack of thin semiconductor wafers are placed in a
lattice within an acoustically reflective chamber. Upon the
addition of electrons, short-wavelength (in the terahertz range)
phonons are produced. Since the electrons are confined to the
quantum wells existing within the lattice, the transmission of
their energy depends upon the phonons they generate. As these
phonons strike other layers in the lattice, they excite
electrons, which produce further phonons, which go on to excite
more electrons, and so on. Eventually, a very narrow beam of
high-frequency ultrasound exits the device.

**Uses**

Apart from allowing the investigation of terahertz-frequency
ultrasound, the SASER is also likely to find a myriad of uses in
optoelectronics, as a method of signal modulation and/or
transmission. [1]

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[**http://www.abovetopsecret.com/forum/thread145379/pg1**](http://www.abovetopsecret.com/forum/thread145379/pg1)

**SASER**

A theoretical scheme of a saser (Sound Amplification by
Stimulated Emission of Radiation) is proposed. A liquid with gas
bubbles is used as the active medium. Pumping is performed with
an alternating electric field or mechanical vibrations of the
resonator. Phase bunching of initially incoherent radiators
(bubbles) occurs under the action of acoustic radiation forces.
The proposed scheme is similar to that of a free-electron laser.
Two models of an active medium are studied. In the first model
it is assumed that all bubbles have the same radius. In the
second model a continuous distribution of bubble radii is
studied. The starting values for sasers with square and
cylindrical resonators are calculated. It is shown that in all
cases studied these conditions are identical, to within a
numerical factor. The operation of a saser in a nonlinear regime
and the directional pattern of a saser in the saturation regime
are studied.

*reply to post by Merkeva*

Use your imagination. You can make somebody miles away hear,
what you want to say. And probably only he hears the sound "in
his head" and nobody else near him.   
And you could brake walls, resonating at the right spots with a
right rythm/amplitude(/wave shape) - from a distance. It can be
also very harmful to the people.

And maybe with that principle you can transmit some quantity of
energy through the air. Ad more: think of leaver and ultrasonic
technology. If they can break stones inside the soft tissue,
maybe they could cause changes on a microlevels of matter being.
Let's say melt a metal without heating it then mixed it with
some liquid. And break stone or ice in the mountains, on a safe
distance. Clean work, cheap too. Very harmful.

And the new era of discoteques... where each wisitor would hear
different music, according to his coordinates/position in the
room. The name could be Music on the spot or something.   
Anyway, there's an interesting stuff on a google video named
Cymatics soundscape. There you can see, what soud does to
matter.

Or better, you see a dance of creative sound and willing
matter.

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[**http://www.physik3.gwdg.de/isna/talk-list-abstracts/V.Kedrinskii.html**](http://www.physik3.gwdg.de/isna/talk-list-abstracts/V.Kedrinskii.html)

**Shock Amplification by System with Energy
Release (SASER)**

**V. Kedrinskii, Yu. Shokin, V. Vshivkov, G.
Dudnikova**

Lavrentyev Institute of Hydrodynamics, Institute of
Computational Technology, Novosibirsk 630090, Russia

The paper is devoted to one of approaches to the solution of
so-called problem of ``Acoustical Laser'' (acoustical analogy of
laser system). In this connection primary attention is focused
on the heterogeneous structure of reactive liquids containing
macroinhomoheneities which can be a main reason of arising such
known phenomena as bubbly detonation and explosion of a
combustible liquids stored under pressure in containers when
they are suddenly depressurized.

One can mention about some analogies of LASER/SASER systems :
1. adiabatic explosion of gas mixture into the bubbles (hot-spot
system formation) of reactive bubbly system can be considered as
a physical analogy of pumping process of laser system; 2. an
energy release during the process of wave propagation above the
hot-spot system and its amplification is an analogy of ``forced
radiation'' effect. Statement features of numerical study
presented consist in that a wave process development both in
passive and reactive bubbly systems as a set of layers is
considered when boundary as well as physical conditions can be
changed for the certain instants of time according to the given
program. In particular the model allows a reactive gas mixture
to be reconstracted after an igniting detonation behind the wave
passed. The calculations have shown that in such kind systems a
pressure can be ``pumped'' up to a rather high level.

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[**http://www3.interscience.wiley.com/journal/109793688/abstract?CRETRY=1&SRETRY=0**](http://www3.interscience.wiley.com/journal/109793688/abstract?CRETRY=1&SRETRY=0)  
**Wiley Interscience**

**Electrically pumped terahertz SASER device
using a weakly coupled AlAs/GaAs superlattice as the gain
medium**

**R. N. Kini \*, N. M. Stanton, A. J. Kent,
M. Henini**

School of Physics and Astronomy, University of Nottingham,
University Park, Nottingham, NG7 2RD UK   
email: R. N. Kini (ppxrnk@nottingham.ac.uk)

\*Correspondence to R. N. Kini, School of Physics and Astronomy,
University of Nottingham, University Park, Nottingham, NG7 2RD
UK

**Abstract** -- We describe an electrically pumped sound
amplification by stimulated emission of radiation (SASER) device
for terahertz frequencies. The gain medium of the device is a
weakly coupled AlAs/GaAs superlattice (SL). It is incorporated
into a multimode acoustic cavity formed between the top (free)
surface of the structure and a second SL acting as a phonon
reflector. We report measurements on a prototype device using
bolometers to detect the emitted phonons. An enhancement of the
phonon emission parallel to the SL growth direction is observed
when the energy drop per period of the gain SL matched the
cavity phonon energy. This was accompanied by a small increase
in device current. We argue that these results provide evidence
that the device is operating as a SASER. ((c) 2004 WILEY-VCH
Verlag GmbH & Co. KGaA, Weinheim)

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[**http://ieeexplore.ieee.org/Xplore/login.jsp?url=/iel5/6852/18412/00849451.pdf?arnumber=849451**](http://ieeexplore.ieee.org/Xplore/login.jsp?url=/iel5/6852/18412/00849451.pdf?arnumber=849451)  
**Ultrasonics Symposium, 1999. Proceedings. 1999 IEEE ; Volume
1, Issue , 1999 Page(s):509 - 511 vol.1**

**Principles of a Mechanical Type Saser**

**Leach, M.F.; Goldsack, D.E.; Kilkenny, C.**

**Summary**: Musical sands, as well as common materials such
as silica gel, emit inordinately intense audible sounds when
sheared by wind, waves or other mechanical means. Hand shaken
laboratory size samples of these materials produce very coherent
beat-like signals, when displayed on an oscilloscope. Frequency
parameters of these patterns have been related to particle size,
and, more surprisingly perhaps, to sand sample size. By
combining these two relationships, a simple method for creating
a source of single frequency sound has been developed. It
consists of filtering musical sands into narrow size fractions
and then tailoring an appropriate size distribution which can be
finely tuned to any given frequency within the frequency range
defined by the whole sample. Thus, the principles for developing
an active device that converts input mechanical energy into a
narrow intense beam of coherent audible sound have been
established

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