WAVES AND PHOTONS – ENTERING TREACHEROUS TERRITORY
Monday, October 20th, 2008
As I have stated repeatedly the inescapable conclusion of light interaction with the retina as explained in this work is that the eye evolved to detect light as a wave and not as photons. The sub-optical wavelength dimensioned nanostructure defined by receptor outer segments operating in femtosecond (10-15 sec) time “quantizes” the interaction forming a “particle” electron that is subsequently used in an electronic image-forming process.
I would speculate that this interaction can be considered the transition point (described in physics as the “Heisenberg cut”) between the classical and quantum views of reality.
Its “wave reality out there” and “quantized particle reality in here” !
It should therefore not be thought that “photons go from place to place” but rather that it is the electromagnetic wave that is translated into what should be termed a quantized event (or, alternatively, “turned into a photon”) by the light-accepting nanostructure of retinal outer segments of the eye.
To be more precise: a.) the retinal nanostructure evolved to interact with the wave nature of electromagnetic radiation, b.)this nanostructure spatially defines the wavelength of the interaction (to three discrete geometrically defined wavelengths in the eye), and, c.) then translates the absorbed energy laterally in the plane of the retina (orthogonal to entrance light direction) using evanescent wave phenomenon and probably a lossless solitonic mechanism to quantum confined electron sites formed by individual receptors. The translation from classical wave to quantized particle is complete.
Seemingly relevant thoughts attributed to Albert Einstein (although I have not yet corroborated these!) are contained in a blog by one Dr. Stanley Alterman (“Stanley’s World” “Optical Waves Wash Photons Aside”).
“Despite his success, Einstein and others at the time, viewed the quanta as “perplexing, pesky, mysterious, and sometimes a maddening quirk in the cosmos.” (*) In particular, was the quanta of light a property of the light in a vacuum or the property of the process of light interacting with other materials? (emphasis mine / GCH)
“Even though Einstein’s equation for the photoelectric effect was proven to be accurate, he found the quanta representation so untenable, that he no longer held it to be true. He wrote, even after the advent of quantum mechanics theory in the 1920’s, near his death, “all these 50 years of pondering have not brought me any closer to answering the question, what are light quanta?” (*) Einstein thus represented to his dying days that “the wave theory of light which operates with continuous spatial function, has worked well in the representation of purely optical phenomena and will probably never be replaced by another theory.” (*)”
ADDED IN SUPPORT OF THE ABOVE:
We must ask a fundamental question: do we ever really detect single photons? - a question that is at the heart of the above discussion (or, in the light of my thoughts the term “photon” should be replaced with a “quantized event”).
I have some experience in this area of research (described below) but I wonder if we have been misleading ourselves in this regard!
I will first discuss the characteristics of the vacuum photomuliplier tube (PMT) and Richard Feynman’s use of this device as indeed a very fundamental detector of single photons basing his entire thesis on statements regarding it.
First a quote from Feynman’s beautiful treatise “QED (Princeton University Press, 1985) p.15:.
(I assume that R.F’s statements reflect and are not at variance with his deeper thinking)
“….where you were probably told something about light behaving as waves. I’m telling you the way it does behave – like particles” (the emphasis is F’s).
And a further quote:
“You might say that it’s just the photomultiplier that detects light as particles, but no, every instrument that has been designed to be sensitive enough to detect weak light has always ended up discovering the same thing: that light is made of particles” (this time the emphasis mine).
And yet another quote (pp.36, 37):
“…but the wave theory cannot explain how the detector makes equally loud clicks as the light gets dimmer.” (again the emphasis again is mine).
It is of note that Feynman in his exposition in QED does not generally differentiate between “weak light detection” and “single photon” detection and often uses these terms interchangeably.
Now….Feynman’s use of the photomultiplier as an example of a “single photon” detector requires elaboration.
I would assert that the photomultiplier tube is actually not a single photon detector but rather a single electron detector.
Each light-generated electron released inside the tube from the surface of the photocathode enters a cascading dynode structure where its signal is amplified by a factor of a few thousand arriving finally at the signal output anode. This is the generality and until a few years ago all that we really know about the process.
It was discovered only some years ago (1960’s?) and quite by surprise that single electron events could be discerned (“counted”) at the output of the device.
How this discovery was made is an interesting story and I believe that I might even have attended an IEEE Nuclear Science symposium in
In essence, an unexpected peak was seen on the low energy electronic “noise tail” appearing at the anode of certain PMT tubes. It could be deduced from the position of this peak that the event that caused it had undergone the highest amplification with it being recognized peak formation indicated that the initiatory events originated from one spatial location. It was quickly seen that this location was the photosurface at the light input cathode of the tube.
The fact that a peak was seen was a spatial effect related to the geometry of the construction of the tube All initiatory events from a uniform surface being subjected to the same gain resulted in the formation of a peak. The detection of single electrons in the PMT is fundamentally the result of the spatial geometry of the PMT!
It then becomes crucial to note that these electronic output signals from the PMT were all of the same size .In essence, a standard or constant pulse height was measured from single electron events.
I will note again the quote from Feynman above:
“…but the wave theory cannot explain how the detector makes equally loud clicks as the light gets dimmer.” (again the emphasis again is mine).
This has been absolutely explained – and it is not single photons but single electrons that yield the standardized output – or in F’s terms “equally loud clicks”.
I should note that single electron response represents the ultimate in sensitivity of this or any detector. One cannot achieve any greater sensitivity. The standard or “equally loud” signal is exactly what one should expect.
And…single electron response – the ultimate sensitivity! – is also characteristic of the light detection centers of the retina and of the photosynthetic organelles of plans and algae.
Now to the subject of a “single photon response” of the PMT. Feynman would have to assume that a 1:1 correspondence must exist between the incidence of a single photon and the release of a single electron into the vacuum of the PMT. This to my knowledge has never been demonstrated either theoretically or experimentally. Quite the contrary, there seemed to be an “anomalous” yield of single electrons released to the number of incident photons. As I remember (and I stand to be corrected) the best that could be discerned was that a statistical number of photons (30?)reslted in the release of a single electron.
What is the physical situation here? The light interaction process within the photosurface of a PMT occurs in an atomically thick “low work function” (i.e. electron emitting) layer that has been vacuum deposited on the inside of the light entrance glass thickness. As I remember, cesium compounds are used but there are others. The physics of this interaction were studied at the time and there seemed to be many troubling aspects to our understanding of the process and, in summary, it was never really understood.
There was certainly not a one-to-one correspondence between a single incident photon and the release of a single electron.
In reality a PMT therefore detects and “counts” single electrons and not single photons.
Finally, focus again on the two separate aspects of the light detection process in a PMT:
a.) Spatial/geometrical concerns are at the basis of identification of the event.
b.) That a constant signal amplitude, Geiger counter-like, “quantization” of the process results for the case of single electron detection.
___________________________________________
I mentioned above that I have had some experience in single electron detection. My research into, what are termed, the silicon “avalanche” photodetector (actually, a “solid state PMT”) at their best possessed electronic gain values approximating a thousand (103). This was not quite sufficient to detect single electrons. Vacuum PMT detectors with the ability to detect single electrons possess gains of perhaps twice this number. We therefore conceived of the idea of replacing the structural dynode structure of the PMT with an avalanche detector for amplifying the single electron released from the vacuum photosurface. A voltage of a thousand volts or so was applied between the photosurface and the avalanche electron-detecting device. This made for a very compact single electron detector that we proposed would ultimately replace some PMT’s. We made the significant single electron response measurement of the device at a Hughes Aircraft facility in San Diega,Ca. I have that curve somewhere and will dig it if proves necessary. I received a U.S. patent for the concept (No. 5,146,296 “Devices for Detecting and/or Imaging Single Photoelectrons”, Sept. 8, 1992). The last time I looked they are now marketed as “Hybrid Photodetectors” by Applied Photonics, Inc. in
A drawing describing the device made at the time:

