Laser induced charge in glass?

AI Thread Summary
Laser-induced charge in glass involves the creation of localized charge gradients within specialized materials, such as silver-containing zinc phosphate glass and silicate glasses. Research indicates that these charges are not electrical but can be trapped within the material, similar to thermal poling processes. Techniques like multiphoton ionization are used to induce photoconductivity, generating charge carriers in various glass types. The distribution and detection of these charges remain topics of inquiry, with ongoing discussions about their sensing methods. Understanding these processes could have implications for advanced material applications.
Tao Tao
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i am just being curious about some details about how laser can induce charges inside a glass bulk? Does anyone else have more knowledge on this?
 
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Tao Tao, Welcome to Physics Forums!

Here are two papers that describe "charges" inside glasses. Note, please, that these are not electrical charges, and that the glass is highly specialized.

"Three-dimensional direct femtosecond laser writing of second-order nonlinearities in glass

In this Letter, we propose another approach to create inside a silver-containing zinc phosphate glass a laser induced frozen charge gradient, similar to the thermal poling process, but localized with three-dimensionality.

The glass used for this study is a photosensitive zinc and gallium phosphate glass (40P2O5 −
55ZnO − 4Ga2O3 − 1Ag2O) containing 1% (mol.%) of silver oxide."

http://www.creol.ucf.edu/Research/Publications/5555.pdf

and

"LASER-INDUCED PHOTOCONDUCTIVITY IN SILICATE GLASSES BY MULTIPHOTON EXCITATION, A PRECURSOR OF DIELECTRIC BREAKDOWN AND MECHANICAL DAMAGE

A Q-switched ruby laser is used to induce photoconductivity in soda glass, fused quartz, and quartz crystal. The number of charge carriers produced per laser pulse of 1027 photons cm−2 s−1 is accounted for by multiphoton ionization of nonbridging oxygens in the silicon oxygen network."

http://www.nrcresearchpress.com/doi/abs/10.1139/p67-317?journalCode=cjp#.UhK5gL7D_Dc
 
I did not know that

laser generating charges? I did not know that.
 
pedro111 said:
laser generating charges? I did not know that.

well, actually, it is laser induces charge in specified materials, and these charges could be trapped inside a small bulk of the material
 
Bobbywhy said:
Tao Tao, Welcome to Physics Forums!

Here are two papers that describe "charges" inside glasses. Note, please, that these are not electrical charges, and that the glass is highly specialized.

"Three-dimensional direct femtosecond laser writing of second-order nonlinearities in glass

In this Letter, we propose another approach to create inside a silver-containing zinc phosphate glass a laser induced frozen charge gradient, similar to the thermal poling process, but localized with three-dimensionality.

The glass used for this study is a photosensitive zinc and gallium phosphate glass (40P2O5 −
55ZnO − 4Ga2O3 − 1Ag2O) containing 1% (mol.%) of silver oxide."

http://www.creol.ucf.edu/Research/Publications/5555.pdf

and

"LASER-INDUCED PHOTOCONDUCTIVITY IN SILICATE GLASSES BY MULTIPHOTON EXCITATION, A PRECURSOR OF DIELECTRIC BREAKDOWN AND MECHANICAL DAMAGE

A Q-switched ruby laser is used to induce photoconductivity in soda glass, fused quartz, and quartz crystal. The number of charge carriers produced per laser pulse of 1027 photons cm−2 s−1 is accounted for by multiphoton ionization of nonbridging oxygens in the silicon oxygen network."

http://www.nrcresearchpress.com/doi/abs/10.1139/p67-317?journalCode=cjp#.UhK5gL7D_Dc



thank you! i will read yours and we can talk about it later. Can that kind of charge in your material be trapped inside? and do you got some idea on how the charges distribute? and how can we see/ sense them?
 
It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.
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