Molecular spectroscopy and structure: LASERS Flashcards

1
Q

What does LASER stand for?

A

light amplification by the stimulated emission of radiation

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2
Q

When was stimulated emission predicted?

A

by Einstein in 1921

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3
Q

When was stimulated emission observed experimentally?

A

1960

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4
Q

What is ‘population inversion’?

A

many molecules in an excited state wait to be stimulated into emission in a cascade or domino-like process

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5
Q

Name the basic components of a laser

A
  • active medium
  • pump
  • optical resonator
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6
Q

What is the active medium?

A

the luminescent material in which the electromagnetic wave is amplified

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7
Q

What is the pump?

A

a source of energy which supplies the initial energy to active medium required to electronically excite the first molecules

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8
Q

What different pumps are there?

A
  • an optical pump is a high intensity light source such as a flash lamp or another laser
  • an electrical pump supplies energy to the active medium by, for example, electrical discharge
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9
Q

What is the optical resonator?

A

it contains the active medium and is essentially a box with a highly reflecting mirror at each end

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10
Q

What is the active species in a ruby laser?

A

Cr3+ in a synthetic sapphire (Al2O3), doped with about 0.5% Cr2O3

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11
Q

How does the laser work?

A

(1) the ruby crystal is illuminated with an intense flash of radiation of the requisite frequency to match the energy gap between the populated level [0] with energy E0 and an initially unpopulated level [1] with energy E1, exciting a number of the Cr3+ ions to level [1]
(2) state [1] in this system rapidly relaxes through a non-radiative process to a long-lived metastable state [2] with energy E. thus a large number of Cr3+ ions end up in state [2]
(3) when one of the ions in [2] naturally emits a photon, this is able to stimulate emission from another ion in level [2]. there are now two photons moving in phase and in the same direction, both of which can stimulate emission from other ions [2] and so the emission is amplified

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12
Q

Why are molecules in [2] metastable?

A

although a molecule in [1] can be stimulated to emit by the pumping light source (ie. it has the correct frequency), the pumping light source is of too high a frequency to stimulate emission from [2]

(4) after a while, there is a large buildup of light (photons) in the cavity, regulated by the pumping of the system

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13
Q

Which photons contribute to lasing?

A

only photons moving along the axis between the mirrors

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14
Q

What would happen if the mirrors were perfectly reflecting the light?

A

the light built up in the cavity would remain trapped

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15
Q

How should the length of the laser cavity be selected?

A

it must be carefully chosen to be an integer number of wavelengths of the laser radiation - otherwise the laser light would interact with itself destructively

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16
Q

What is the problem with this process?

A
  • each photon emitted from [2] can either be lost at non-reflective surfaces, lead to stimulated emission of another photon from [2] or be absorbed by a molecule in [0] taking it to state 2
  • hence the process of stimulated emission is in direct competition with the process of absorption
17
Q

What is the requirement for population inversion?

A

in order for stimulated emission to outweight absorption, level [2] must have a higher population than [0]

18
Q

For the three-level system described here, what proportion of molecules must be excited to [2] for population inversion to be achieved?

A

if more than half the molecules in the active medium are excited to [2]

19
Q

What is the solution to these problems?

A

the 4-level laser:

  • molecules are excited to [1] by pumping with a flash lamp or just a powerful continuum lamp (ie. continuous pumping)
  • ions cross to a metastable state [2]
  • stimulated emission occurs to an intermediate state [3] (not the ground state)
  • [3] is then immediately depopulated non-radiatively to the ground state [0]
20
Q

What are the advantages of a 4-level laser?

A
  • as the population inversion is between two excited states, it is much easier to achieve and control than a population inversion between an excited state and a heavily populated ground state
  • the lower level of the lasing transition ( [3] in the example given) is very rapidly depopulated and so it is easy to maintain an excess population in the upper lasing level [2]. this means that much lower levels of pumping are needed in order for a population inversion to be sustained
  • the laser can be operated continuously, giving out a continuous wave and the pumping transition can be provided by a continuous light source
  • conversion efficiencies are very much higher
21
Q

Give two examples of organic species with electronic states ideally spaced to allow for their use in 4-level lasers

A

rhodamine 6G and rhodamine B

22
Q

What is the effect of incorporating a diffraction grating?

A
  • the laser light can be tuned to produce a specific frequency within the range of energy levels, corresponding to just one of the vibrational levels of [3]
  • thus we now have a continuum of frequencies available which can be chosen by careful tuning of the laser cavity
23
Q

Why do high power dye lasers need effective stirring and cooling?

A

high power dye lasers need effective stirring and cooling as level [3] is rapidly depopulated by collisions with the solvent molecules, which would otherwise lead to rapid heating of the laser

24
Q

What are the properties of laser light?

A
  • highly monochromatic - all the energy is concentrated in essentially a single frequency
  • radiation is coherent, meaning that the oscillations of the light waves are all in phase with one another
  • radiation is highly parallel. this enables the laser light to be focussed to a very small spot, giving extremely high localised power density
  • pulsed lasers, eg. ruby, can give radiation in extremely small pulses - nowadays shorter than 10^-15 s. this allows for techniques such as femtosecond spectroscopy, which directly probe the vibrations of bonds within molecules
25
Q

At what frequency does the ruby laser emit at?

A

694 nm