that from one photon two is gotten so we can amplify light.
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L
is distance between mirrors, m is integer.
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First step for Laser creation
Absorption: When electrons in the ground state absorb a photon with certain energy then it can move to a higher state, if the energy difference between ground and excited state is same as photons energy.
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Spontaneous emission
The electron goes back to the ground state after some time and emits a photon of defined energy.
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Population inversion
To get a high intensity light we need to create a lot of numerous excited electrons in a material then invest energy from outside into the material (laser pumping)
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Stimulated emission
Einstein that we could induce emission, when a photon with energy that satisfies Bohrs condition for electrons in excited state is emitted by electron in excited state.
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LASER
Light amplification by stimulated emission of radiation
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Example of three level system
Ruby laser, the medium is chromium doped synthetic sapphire
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What do we need for Laser oscillators?
gain medium, intensive electron excitation, positive feedback and optical resonator.
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Resonance condition?
2L = m(wavelength)
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Explain Monochromatic attribute of Laser
narrow bandwidth
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Coherence of Lasers?
create interference even in big path differences.
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How is laser Collimated
Has a narrow beam with little divergence
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What is Power density for laser lights
has higher power density (E/At) than ordinary light
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How is laser polarized?
ultrashort pulses
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Pulse length of Q-switched lasers
100 - 200ns
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Example of 4 level system
He-Ne laser
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Classification of lasers
By gain medium, by operation and by energy
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Types of lasers by operation
Pulse lasers and continuous wave
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Comparison of pulse lasers and continuous wave
Pulse lasers produce series of pulses at certain width and frequency until stopped
Continuous wave releases constant output over interval of seconds
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Medical application of Lasers
Surgical operations, retinal laser surgery, gene surgery
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Metastable state
Short lived high energy state that spontaneously drops to a low energy state with long lifespan
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How to achieve laser pumping
Thermal excitation, optical excitation and electric discharge