[Vo]:Re: Optics, magnetics spinplasmonics

2014-04-25 Thread Mark Jurich


Bob Cook wrote:

| I am about 2/3 through the paper you identified on the transmission 
of a
| terahertz electric field wave form through Ni and Co particles  in a 
static

| magnetic field.

... Just to clarify, this is a reference that Jones cited and I just gave a 
link to it that wasn't behind a pay wall.  Perhaps Jones may comment also to 
your questions...


| Does the oscillating terahertz electric field produce a perpendicular
| oscillating magnetic field?  Or does that only happen with  photon
| propagation?

Yes it does.  The Terahertz Electromagnetic Field is a photon field, and 
it will induce a magnetization.  This is a very weak H Field compared to the 
applied static magnetic field, but the localized magnetic field strength 
would depend on any amplification produced by the generation of the Surface 
Plasmon-Polariton (SPP) or whatever quasi-particle coupling might occur...


| Would a terahertz  laser have a different effect?  And would you see
| a phase change in the transmission of the beam through the Ni and Co
| particles?

My guess is that a Terahertz (THz) Laser (being more intense) would increase 
the effect.  The technique used in the paper is indeed sensitive to phase 
changes.  The THz pulse-induced phase change of the probe beam is converted 
into an intensity modulation.  They are using a Ti:sapphire Mode-Locked 
Laser to initially generate the pulse beam fed into the THz Emitter and the 
probe beam.  I'm not sure I'm addressing your question, here.  Perhaps you 
can elaborate...


| If the changing electric field does in fact cause a changing magnetic 
field,

| it would seem that it may introduce some impedence in the transfer of
| the electric field and account for the slight unexplained phase 
change
| reported with respect to the electric field wave form after passing 
through

| the film of the particle assemblege.

... I'm not sure it's possible to disagree with your statements above.  Can 
you possibly point to the unexplained phase shift that you are referring to, 
so that I may comment?  I believe they see a phase shift for both uncoated 
and coated microparticles.  Are you referring to all of the results, given? 
The THz Probe Pulse is 800 nm Wavelength and could be exciting SPPs, 
optically (vs. Terahertz) if I understand the setup correctly.  Here is a 
link to Ref. 19 which describes the experimental setup (hopefully you can 
get to the paper):


http://www.opticsinfobase.org/oe/abstract.cfm?uri=oe-17-8-6600

| Do you know what the N metal film is that the authors stated was 
applied
| to the Ni and Co particles in discussing the experimental set-up? 
Should

| that be no metal film?

N-Metal Film in this case, refers to Nonmagnet Film (or Non-Ferromagnetic or 
Normal vs. Ferromagnetic, F).  This can be very confusing because 
hard-core Plasmonic people sometimes refer to N-Metal Films as Noble Metal 
Films (which are extensively used in the paper), but if they were to mention 
it this way they would be very clear about it, unlike Spin Freaks (just 
kidding!).


- Mark Jurich 



RE: [Vo]:Re: Optics, magnetics spinplasmonics

2014-04-25 Thread Jones Beene
Mark and Bob probably got more out of this paper than I did. However, this 
article from Physics Web about Negative resistance in a 2D electron gas may 
answer one question (about how growing impedance is avoided in spinplasmonics)

http://www.intalek.com/Index/News/PhysicsWeb%20-%20Negative%20resistance%20found%20in%202D%20electron%20gas.htm

Spinplasmonics, as I understand it, would be a 2D phenomenon which can force a 
1D reaction. The detail that seems to be most applicable to a spinplasmonics 
explanation for LENR would be where there is IR semi-coherency in the reactor 
(instead of having a laser, as in the paper). We have called this triple 
coherency in the past although it is more like superradiance than real 
coherence. 

This would replace a laser with internal wave alignment of light (photons), 
magnetism (electron spin), and temperature (phonon excursion); where we seem to 
be setting the stage for gain with dense hydrogen as the exchange medium. The 
most feasible frequency that triple coherency can operate at is the tens of 
THz, since temperature is the defining limitation.

The resultant gain could be nuclear, but it does not have to be if there is an 
easier route based on pushing formerly 3D particles into 1-space via triple 
coherency. 

If the particle is the DDL state of hydrogen, which has an effective magnetic 
field in the millions of Tesla, then spinplasmonics seems to accomplish this 
task elegantly via spin coupling.

(which pleases the spin freaks :)


-Original Message-
From: Mark Jurich 

 Bob Cook wrote:

 | I am about 2/3 through the paper you identified on the transmission 
of a
 | terahertz electric field wave form through Ni and Co particles  in a 
static
 | magnetic field.

... Just to clarify, this is a reference that Jones cited and I just gave a 
link to it that wasn't behind a pay wall.  Perhaps Jones may comment also to 
your questions...

 | Does the oscillating terahertz electric field produce a perpendicular
 | oscillating magnetic field?  Or does that only happen with  photon
 | propagation?

Yes it does.  The Terahertz Electromagnetic Field is a photon field, and 
it will induce a magnetization.  This is a very weak H Field compared to the 
applied static magnetic field, but the localized magnetic field strength 
would depend on any amplification produced by the generation of the Surface 
Plasmon-Polariton (SPP) or whatever quasi-particle coupling might occur...

 | Would a terahertz  laser have a different effect?  And would you see
 | a phase change in the transmission of the beam through the Ni and Co
 | particles?

My guess is that a Terahertz (THz) Laser (being more intense) would increase 
the effect.  The technique used in the paper is indeed sensitive to phase 
changes.  The THz pulse-induced phase change of the probe beam is converted 
into an intensity modulation.  They are using a Ti:sapphire Mode-Locked 
Laser to initially generate the pulse beam fed into the THz Emitter and the 
probe beam.  I'm not sure I'm addressing your question, here.  Perhaps you 
can elaborate...

 | If the changing electric field does in fact cause a changing magnetic 
field,
 | it would seem that it may introduce some impedence in the transfer of
 | the electric field and account for the slight unexplained phase 
change
 | reported with respect to the electric field wave form after passing 
through
 | the film of the particle assemblege.

... I'm not sure it's possible to disagree with your statements above.  Can 
you possibly point to the unexplained phase shift that you are referring to, 
so that I may comment?  I believe they see a phase shift for both uncoated 
and coated microparticles.  Are you referring to all of the results, given? 
The THz Probe Pulse is 800 nm Wavelength and could be exciting SPPs, 
optically (vs. Terahertz) if I understand the setup correctly.  Here is a 
link to Ref. 19 which describes the experimental setup (hopefully you can 
get to the paper):

http://www.opticsinfobase.org/oe/abstract.cfm?uri=oe-17-8-6600

 | Do you know what the N metal film is that the authors stated was 
applied
 | to the Ni and Co particles in discussing the experimental set-up? 
Should
 | that be no metal film?

N-Metal Film in this case, refers to Nonmagnet Film (or Non-Ferromagnetic or 
Normal vs. Ferromagnetic, F).  This can be very confusing because 
hard-core Plasmonic people sometimes refer to N-Metal Films as Noble Metal 
Films (which are extensively used in the paper), but if they were to mention 
it this way they would be very clear about it, unlike Spin Freaks (just 
kidding!).

- Mark Jurich 



RE: [Vo]:Re: Optics, magnetics spinplasmonics

2014-04-25 Thread Roarty, Francis X
Works pretty well for Zero Point people too!

-Original Message-
From: Jones Beene [mailto:jone...@pacbell.net] 
Sent: Friday, April 25, 2014 10:01 AM
To: vortex-l@eskimo.com
Subject: EXTERNAL: RE: [Vo]:Re: Optics, magnetics  spinplasmonics

Mark and Bob probably got more out of this paper than I did. However, this 
article from Physics Web about Negative resistance in a 2D electron gas may 
answer one question (about how growing impedance is avoided in spinplasmonics)

http://www.intalek.com/Index/News/PhysicsWeb%20-%20Negative%20resistance%20found%20in%202D%20electron%20gas.htm

Spinplasmonics, as I understand it, would be a 2D phenomenon which can force a 
1D reaction. The detail that seems to be most applicable to a spinplasmonics 
explanation for LENR would be where there is IR semi-coherency in the reactor 
(instead of having a laser, as in the paper). We have called this triple 
coherency in the past although it is more like superradiance than real 
coherence. 

This would replace a laser with internal wave alignment of light (photons), 
magnetism (electron spin), and temperature (phonon excursion); where we seem to 
be setting the stage for gain with dense hydrogen as the exchange medium. The 
most feasible frequency that triple coherency can operate at is the tens of 
THz, since temperature is the defining limitation.

The resultant gain could be nuclear, but it does not have to be if there is an 
easier route based on pushing formerly 3D particles into 1-space via triple 
coherency. 

If the particle is the DDL state of hydrogen, which has an effective magnetic 
field in the millions of Tesla, then spinplasmonics seems to accomplish this 
task elegantly via spin coupling.

(which pleases the spin freaks :)


-Original Message-
From: Mark Jurich 

 Bob Cook wrote:

 | I am about 2/3 through the paper you identified on the transmission 
of a
 | terahertz electric field wave form through Ni and Co particles  in a 
static
 | magnetic field.

... Just to clarify, this is a reference that Jones cited and I just gave a 
link to it that wasn't behind a pay wall.  Perhaps Jones may comment also to 
your questions...

 | Does the oscillating terahertz electric field produce a perpendicular
 | oscillating magnetic field?  Or does that only happen with  photon
 | propagation?

Yes it does.  The Terahertz Electromagnetic Field is a photon field, and 
it will induce a magnetization.  This is a very weak H Field compared to the 
applied static magnetic field, but the localized magnetic field strength 
would depend on any amplification produced by the generation of the Surface 
Plasmon-Polariton (SPP) or whatever quasi-particle coupling might occur...

 | Would a terahertz  laser have a different effect?  And would you see
 | a phase change in the transmission of the beam through the Ni and Co
 | particles?

My guess is that a Terahertz (THz) Laser (being more intense) would increase 
the effect.  The technique used in the paper is indeed sensitive to phase 
changes.  The THz pulse-induced phase change of the probe beam is converted 
into an intensity modulation.  They are using a Ti:sapphire Mode-Locked 
Laser to initially generate the pulse beam fed into the THz Emitter and the 
probe beam.  I'm not sure I'm addressing your question, here.  Perhaps you 
can elaborate...

 | If the changing electric field does in fact cause a changing magnetic 
field,
 | it would seem that it may introduce some impedence in the transfer of
 | the electric field and account for the slight unexplained phase 
change
 | reported with respect to the electric field wave form after passing 
through
 | the film of the particle assemblege.

... I'm not sure it's possible to disagree with your statements above.  Can 
you possibly point to the unexplained phase shift that you are referring to, 
so that I may comment?  I believe they see a phase shift for both uncoated 
and coated microparticles.  Are you referring to all of the results, given? 
The THz Probe Pulse is 800 nm Wavelength and could be exciting SPPs, 
optically (vs. Terahertz) if I understand the setup correctly.  Here is a 
link to Ref. 19 which describes the experimental setup (hopefully you can 
get to the paper):

http://www.opticsinfobase.org/oe/abstract.cfm?uri=oe-17-8-6600

 | Do you know what the N metal film is that the authors stated was 
applied
 | to the Ni and Co particles in discussing the experimental set-up? 
Should
 | that be no metal film?

N-Metal Film in this case, refers to Nonmagnet Film (or Non-Ferromagnetic or 
Normal vs. Ferromagnetic, F).  This can be very confusing because 
hard-core Plasmonic people sometimes refer to N-Metal Films as Noble Metal 
Films (which are extensively used in the paper), but if they were to mention 
it this way they would be very clear about it, unlike Spin Freaks (just 
kidding!).

- Mark Jurich 



Re: [Vo]:Re: Optics, magnetics spinplasmonics

2014-04-25 Thread Mark Jurich


Mark Jurich wrote:

| The THz Probe Pulse is 800 nm Wavelength and could be
| exciting SPPs, optically (vs. Terahertz) if I understand the
| setup correctly.  Here is a link to Ref. 19 which describes
| the experimental setup (hopefully you can get to the paper):

| http://www.opticsinfobase.org/oe/abstract.cfm?uri=oe-17-8-6600

You idiot, look at Fig. 1 in Ref. 19 better and you will see that the Probe 
Pulse doesn't go through the Sample, so 800 nm radiation should never make 
it there, especially if one places a 800 nm Optical Rejection filter in the 
path! :)


... Table II is still puzzling with respect to the flip between Ni/Ag - 
Ni/Al Attenuation and Co/Ag - Co/Al Attenuation.  Somehow, I would expect 
the Ni Values to be correct and the Co ones to be the ones out of place...


Here are some crude e1/e2 Optical Constants I dug up, at the 0.75 THz Region 
(25 cm-1 (wavenumbers), or 400 um):


Ni:e1: -6E4 e2: 3E5

Au:   e1: -8.6E4  e2: 6.2E5
Ag:   e1: -3E5 e2: 1.5E6
Al:e1: -3E4 e2: 1E6

where e = e1 + i e2 .

... I'm still searching for the Co Values...

FYI: Here is a link to their earlier PRL Paper when they first introduced 
their Spintronic-Plasmonic Cobalt Media:


http://www.physics.gla.ac.uk/~dtngo/Article/PRL_98_133901_2007.pdf

The above paper mentions Co:  e1: -1E5 .

... Have fun, Spintronicating!

- Mark Jurich