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Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser

Physics

Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser

Overview

Overview

🌳 Concept tree

Lesson 1→Laser Physics, Population Inversion and the Helium-Neon Laser

├── Energy levels and transitions

  • ├── Comparison between spontaneous and stimulated emission

├── Worked examples (Lesson 1)

├── Properties of the laser beam

├── Monochromaticity (spectral purity)

├── Collimation (a parallel narrow beam)

├── Coherence

├── Intensity (concentration)

├── Worked examples (Lesson 2)

├── Population inversion

├── The three essential elements of any laser

├── Laser action step by step

├── Worked examples (Lesson 3)

├── Construction

├── Operation

├── Applications of lasers

├── Holography (3-D photography)

├── Medicine

├── Other applications

├── Why a threshold? (gain versus loss)

├── Continuous and pulsed operation

├── A guide to common lasers

├── Eye safety and classes

├── Photon arithmetic for laser problems

  • ├── Typical exam questions and model answers (outline)

├── Chapter summary

└── Common mistakes

Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 1 / 33
Energy levels and transitions

Energy levels and transitions

  • An atom can exist only in certain energy states.
  • The lowest is the ground state (E₁), in which the atom is normally found.
  • The atom can be raised to higher states E₂, E₃, …
  • (excited states).
  • Three processes can occur between two levels E₁ and E₂:
  • (a) Absorption (excitation). A photon of energy hν = E₂ − E₁ falls on an atom in the ground state. The atom absorbs the photon and the electron rises to the level E₂. The atom can also be excited by a collision with an electron or another atom, by an electric discharge or by heat.
  • (b) Spontaneous emission. The excited atom stays in the level E₂ for only a short time, its lifetime (about 10−8 s). After this, with no external influence, it returns to E₁ by emitting a photon of energy hν = E₂ − E₁. This is the radiation in ordinary light sources (lamps, flames, the Sun). The photons from different atoms are emitted at random times, in random directions and with random phases: the light is incoherent and spreads out.
(c) Stimulated emission.→In 1917 Einstein showed that another process exists. If a photon of energy hν = E₂ − E₁ passes near an atom that is already excited (in E₂) before its lifetime is over, it can force the atom to drop to E₁ at once, releasing a second photon. The new photon is a perfect copy of the incident one: it has the same frequency (energy), the same phase and the same direction. Now two photons move together, in step. If they meet other excited atoms, four photons are produced, then eight, and so on: this is amplification of light. Stimulated emission is the dominant process in a laser.
Comparison aspectMain ideaKeywords
•
  • The incident photon is not absorbed in this process
  • it continues
  • together with the new photon
incidentphotonabsorbedprocess
(Absorption and stimulated emission compete
  • a photon passing a ground-state atom may be absorbed
  • a photon passing an excited atom may stimulate emission
photonpassinggroundstate
To amplify, excited atoms must outnumber ground-state atomsthis is the population inversion discussed in Lesson 3.)populationinversiondiscussedLesson
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 2 / 33
Comparison between spontaneous and stimulated emission

Comparison between spontaneous and stimulated emission

Comparison aspect Spontaneous emission Stimulated emission
How it occurs
  • the excited atom drops to a lower level by itself after its lifetime
  • with no external photon
an external photon of energy E₂ − E₁ makes the excited atom drop before its lifetime ends
Photons emitted random in time, direction and phase
  • same frequency
  • phase and direction as the stimulating photon
Wavelengths
  • a range of wavelengths (many transitions
  • broad lines)
a single wavelength (monochromatic)
Coherence incoherent coherent
Propagation
  • spreads out in all directions
  • intensity falls with the inverse-square law (spreading) and with scattering
  • a narrow
  • parallel beam
  • the intensity remains almost constant over long distances (it has been sent to the Moon and back)
Where it dominates ordinary light sources laser sources
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 3 / 33
Worked examples (Lesson 1)

Worked examples (Lesson 1)

  • Example 1.1 — Photon needed. An atom has levels E₁ = 0 and E₂ = 1.96 eV. What photon is needed for excitation, and what are the properties of a photon released by stimulated emission?
  • hν = 1.96 eV, λ = 1240/1.96 = 633 nm (red).
  • The stimulated photon has the same 633 nm wavelength, travels in the same direction and in phase with the stimulating photon.
  • Example 1.2 — Amplification. One photon passes along a column of excited atoms. If every photon stimulates one new photon in each pass (doubling), how many photons after 10 passes? 210 = 1024 photons, all coherent. After 20 passes: more than a million. This shows the idea of the "chain reaction" of stimulated emission (in a real laser, losses such as the mirror leak reduce the gain).
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 4 / 33
Properties of the laser beam

Properties of the laser beam

  • A laser beam has four properties that distinguish it from ordinary light.
  • All of them come from the fact that the photons are produced by stimulated emission.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 5 / 33
Monochromaticity (spectral purity)

Monochromaticity (spectral purity)

  • Each spectral line of an ordinary source is not a single wavelength: it has a width (a band of wavelengths with different intensities), which is why even a "pure" colour from a lamp shows slightly different shades.
  • A laser emits one extremely narrow spectral line, the intensity being concentrated at one wavelength.
  • The laser is therefore called monochromatic.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 6 / 33
Collimation (a parallel narrow beam)

Collimation (a parallel narrow beam)

  • In an ordinary source the beam widens as it moves away; the energy spreads over a larger and larger area.
  • The diameter of a laser beam remains almost constant for long distances, because all photons move in the same direction.
  • A laser beam can therefore carry energy over long distances without much loss.
  • For example, a laser beam sent to a reflector placed on the Moon’s surface (about 380 000 km away) returns to the Earth, and the time of the round trip gives the distance accurately.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 7 / 33
Coherence

Coherence

  • Photons of an ordinary source are emitted at random instants with random phases.
  • In a laser the photons are emitted together, with the same phase, and keep a constant phase difference while travelling (coherence in time and in place).
  • This allows interference to be observed over large distances and makes the beam intense and focusable.
  • Coherence is the property that makes holography possible.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 8 / 33
Intensity (concentration)

Intensity (concentration)

  • For an ordinary source, the intensity at a distance r from a small source is P/4πr2, so it falls according to the inverse-square law, because of spreading (and scattering by particles).
  • A laser’s energy is concentrated in a small cross-section and the beam is practically unspread, so the intensity per unit area stays almost constant (not subject to the inverse-square law).
  • Even a laser of milliwatt power has a much higher intensity than a lamp of the same power.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 9 / 33
Worked examples (Lesson 2)

Worked examples (Lesson 2)

Comparison aspectMain ideaKeywords
Example 2.1 — Intensity comparison.A 5 mW laser beam has a cross-section of radius 1 mm. An ordinary point source of the same power radiates in all directions. Compare their intensities at 10 mlaserbeamcrosssection
LaserI = P/A = 5 × 10−3 / (π × (10−3)2) = 1.6 × 103 W/m2. Point source at 10 m: I = P/(4πr2) = 5 × 10−3/(4π × 100) = 4.0 × 10−6 W/m2. The laser’s intensity is about 4 × 108 times greaterPointsource4πr2intensity
Example 2.2 — Moon ranging.
  • A pulse sent to the Moon’s reflector takes how long to come back? Distance 3.84 × 108 m: t = 2d/c = 2 × 3.84 × 108/3 × 108 = 2.56 s. If the time can be measured to 1 nanosecond
  • the distance is known to 15 cm (2d = ct)
pulsesentreflectortakes
Example 2.3 — Inverse-square law.→The intensity of an ordinary lamp at 1 m is 400 W/m2. At 4 m it is 400/16 = 25 W/m2. A laser beam’s intensity at 4 m is unchanged.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 10 / 33
Population inversion

Population inversion

  • In ordinary conditions (thermal equilibrium) most atoms are in the ground state, and only a few are excited.
  • A photon passing through the material is therefore usually absorbed.
  • For net amplification by stimulated emission, the number of atoms in the excited state must exceed the number in the lower state.
  • This unnatural situation is called population inversion.
  • It does not occur by itself energy must be supplied to the material continuously (pumping), and the atoms must be of a kind that can stay excited long enough.
  • Metastable states.
  • Population inversion is usually obtained through a metastable level, an excited level with a relatively long lifetime (about 10−3 s instead of 10−8 s).
  • The atoms are pumped to a higher short-lived level; they fall quickly (without radiation or with heat) to the metastable level, where they accumulate.
  • As the atoms leave the metastable level slowly while others arrive quickly, the metastable level becomes more crowded than the lower level, and population inversion is reached.
  • This scheme is called a three-level (or four-level) system.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 11 / 33
The three essential elements of any laser

The three essential elements of any laser

  • Although lasers differ in size, type and wavelength, all have:
  • 1) An active medium. The material in which population inversion is achieved. It may be:

a crystalline solid (e.g. ruby),

a semiconductor,

a liquid dye,

a gas of atoms (e.g. He-Ne),

an ionised gas (e.g. argon),

  • a gas of molecules (e.g. CO₂).
  • 2) An energy source (pumping) to excite the atoms of the medium:
Comparison aspectMain ideaExampleKeywords
(a) Electrical excitation
  • by radio-frequency waves or by an electric discharge under a high DC voltage
  • used in gas lasers (He-Ne
  • argon
  • CO₂)
—radiofrequencywavesdischarge
(b) Optical pumping
  • by light
  • either from a flash lamp (ruby laser) or from another laser (dye laser)
—lighteitherflashlamp
(c) Thermal excitationby collisions of gas atoms having large kinetic energy (as in the He-Ne laser the helium atoms transfer energy by collision)—collisionsatomshavinglarge
(d) Chemical excitationby chemical reactions that release energy to the atoms (
  • hydrogen with fluorine
  • or deuterium fluoride with CO₂)
reactionsreleaseenergyatoms
•3) A resonant cavity—resonantcavity
  • (an optical resonator) that makes the beam bounce to and fro through the active medium so that the amplification builds up.
  • It can be:
Comparison aspectMain ideaKeywords
(a) an external cavitytwo parallel mirrors on either end of the active medium (as in gas lasers)parallelmirrorseitheractive
(b) an internal cavity
  • the two ends of the active rod are polished and coated to act as mirrors (as in the ruby laser). One of the two mirrors is partially transparent (semitransparent)
  • to let a part of the radiation leak out as the output laser beam
  • the other mirror reflects almost 100 %
endsactivepolishedcoated
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 12 / 33
Laser action step by step

Laser action step by step

  1. The pump raises many atoms of the active medium to excited levels, and, through a metastable level, produces a population inversion.
  2. Some atoms decay spontaneously, emitting photons in all directions. Photons that do not travel along the axis leave the sides of the tube and are lost.
  3. Photons travelling along the axis stimulate other excited atoms to emit identical photons. These photons are reflected by the mirrors and pass again and again through the medium, causing new stimulated emission each time. The number of identical photons grows (amplification).
  4. When the beam becomes strong enough, a fraction leaves through the semitransparent mirror as the laser beam. The rest remains in the cavity to continue stimulating atoms.
  5. Meanwhile the pump keeps refilling the excited level, so the process continues.
  • Why is the resonant cavity needed?
  • It makes the photons pass through the medium many times, which increases the number of stimulated emissions (amplification) and also selects only the photons that travel along the axis, thereby giving a narrow, parallel, coherent beam.
  • Why must the active medium be in population inversion for a laser, but not for an ordinary lamp? In a lamp, light comes from spontaneous emission and needs no amplification.
  • In a laser, amplification by stimulated emission must beat absorption; this is possible only if excited atoms outnumber unexcited ones.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 13 / 33
Worked examples (Lesson 3)

Worked examples (Lesson 3)

Comparison aspectMain ideaKeywords
Example 3.1 — Output of the semitransparent mirror.
  • The mirrors of a laser have reflectances of 99.5 % and 98 %. What fraction of the light survives one complete round trip (a pass in each direction and a reflection at each mirror)
  • ignoring the gain? 0.995 × 0.98 = 0.975. After 10 round trips: 0.97510 = 0.78. The gain of the medium must compensate for the losses (mainly through the output coupling) for the laser to operate
mirrorslaserreflectancesWhat
Example 3.2 — Pump efficiency.
  • A He-Ne laser takes 20 W of electrical power and gives 5 mW of light. Efficiency = 5 × 10−3/20 = 2.5 × 10−4 = 0.025 %. The rest is heat. Gas lasers are inefficient
  • the laser is valuable for the quality of light
  • not the efficiency
lasertakeselectricalpower
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 14 / 33
Construction

Construction

  • A quartz glass tube containing a mixture of helium and neon gases in the ratio 10 : 1 at a low pressure of about 0.6 mm Hg.
  • At the two ends of the tube are two parallel mirrors perpendicular to the axis: one has a reflection coefficient about 99.5 %, the other is semitransparent (reflection about 98 %), from which the laser beam leaves.
  • A source of high-frequency electric field outside the tube, or a high DC voltage between two electrodes inside, produces an electrical discharge in the gas.
  • Why helium and neon?
  • The laser light comes from neon, the active atoms.
  • Helium is added because one of its metastable excited levels has almost exactly the same energy as one of the metastable levels of neon.
  • Helium atoms are excited easily by the discharge, and since they are ten times more numerous they transfer energy to neon atoms efficiently by collisions (resonant energy transfer).
  • Thus helium acts as the energy "pump" for neon, and is the reason the population inversion of neon can be achieved.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 15 / 33
Operation

Operation

  1. The electrical discharge accelerates electrons, which collide with helium atoms and excite them to their metastable levels (long lifetime), where they accumulate.
  2. An excited helium atom collides with a neon atom in the ground state and gives it its energy; because the two energy levels are nearly equal, the neon atom is excited to its metastable level. (Helium returns to the ground state.)
  3. The neon atoms accumulate in this metastable level, which has a relatively long lifetime (about 10−3 s), so the number of neon atoms there exceeds the number in the lower level: population inversion.
  4. Some neon atoms fall spontaneously to a lower level, emitting photons of energy equal to the difference between the two levels (633 nm, red light). These photons go in all directions; those along the axis are reflected by the mirrors.
  5. While moving to and fro between the mirrors, these photons collide with other excited neon atoms and stimulate them to emit identical photons: the number of photons doubles again and again (amplification).
  6. When the intensity is high enough, a part leaves through the semitransparent mirror as the laser beam; the remaining part stays inside to continue stimulating.
  7. The neon atoms that have fallen to the lower level lose the rest of their energy by collisions with the walls and other atoms and return to the ground state, where they are ready for helium to excite them again. Helium atoms which lost energy are excited again by the discharge.
  • The He-Ne laser transforms electrical energy into optical energy (and heat).
  • Its most common wavelength is 632.8 nm (red); the beam is continuous with power of a few milliwatts.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 16 / 33
Applications of lasers

Applications of lasers

  • The laser spectrum extends over the visible, ultraviolet and infrared regions.
  • Some lasers focus enough energy into a tiny spot to melt and evaporate iron or drill diamonds; others are powerful enough to be used in military research (destroying missiles).
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 17 / 33
Holography (3-D photography)

Holography (3-D photography)

  • An ordinary photograph records only the intensity (amplitude squared) of the light from different points of the object, so it is a flat (2-D) picture. It loses information about the phase, which depends on the path length from each point of the object, i.e. on the depth and surface relief of the object (phase difference = 2π/λ × path difference).
  • In 1948 the Hungarian scientist Dennis Gabor (Nobel Prize) suggested recording the missing information by interference. A coherent beam is divided into two: one beam illuminates the object and reaches the photographic plate carrying information (the object beam); the other falls directly on the plate (the reference beam), with the same wavelength. The two beams interfere on the plate, and the developed plate shows a complicated pattern of fringes, the hologram. It contains both amplitude and phase information.
  • To view, the hologram is illuminated by the reference beam (laser light of the same wavelength). It acts as a grating and reconstructs the original light waves; the observer sees a complete three-dimensional image of the object, with depth and parallax (different views from different positions), without lenses.
  • A laser is essential because the two beams must be coherent to produce stable interference fringes.
Applications of holograms→security marks on banknotes and cards, art, data storage, testing the stress of components by hologram interferometry.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 18 / 33
Medicine

Medicine

Comparison aspectMain ideaKeywords
Retinal detachment
  • if parts of the retina separate from the layer beneath it
  • they lose their function
  • repair must be fast. A thin laser beam is passed through the pupil to the damaged region
  • its heat welds the retina to the layer below in a fraction of a second
  • saving the sight. Previously this needed a long
  • complicated operation
partsseparatelayerbeneath
Vision correctionlasers reshape the cornea to treat short and long sight (myopia and hypermetropia) and remove the need for glasseslasersreshapecorneatreat
Endoscopylaser beams carried by optical fibres are used inside the body for diagnosis and surgery with minimum cuttinglaserbeamscarriedoptical
Other uses
  • bloodless surgery (the heat seals blood vessels)
  • removing tumours and skin marks
  • dentistry
bloodlesssurgeryheatseals
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 19 / 33
Other applications

Other applications

Comparison aspectMain ideaKeywords
Communications
  • laser beams guided in optical fibres replace telephone cables
  • carrying huge amounts of information with little loss
laserbeamsguidedoptical
Industry
  • precision cutting
  • welding
  • drilling and measurement
precisioncuttingweldingdrilling
Military
  • guiding missiles (the target is lit with a laser
  • and the missile follows the reflected beam: the narrow beam gives precision)
  • range-finding and laser radar (LADAR)
guidingmissilestargetlaser
Compact discs (CDs/DVDs)a laser burns and reads microscopic pitslaserburnsreadsmicroscopic
Laser printers
  • a laser beam writes the page image onto a light-sensitive drum
  • toner is attached and transferred to paper
beamwritespageimage
Arts and showslaser light showslaserlight
Surveying
  • accurate measurement of distances
  • areas and levels
accuratemeasurementdistancesareas
Space researchmeasuring the Earth-Moon distance and the motion of satellitesmeasuringEarthMoondistance
•
  • Barcode scanners
  • laser pointers
  • optical sensors
Barcodescannerslaserpointers
Comparison aspectMain ideaKeywords
Why is a laser used in missile guidance?
  • Its beam is narrow
  • parallel
  • and stays concentrated over long distances
  • therefore it can mark a small target exactly
  • and its single wavelength can be separated from the background light by a filter in the missile’s seeker
beamnarrowparallelstays
Safety
  • a strong laser beam can damage the retina permanently
  • never look into a laser beam or its reflection
stronglaserbeamdamage
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 20 / 33
Why a threshold? (gain versus loss)

Why a threshold? (gain versus loss)

  • A laser does not start working as soon as some atoms are excited.
  • Each time the beam crosses the medium it gains intensity from stimulated emission (gain), and at each round trip it loses intensity through the transmitting mirror (the useful output), absorption and scattering in the cavity (losses).
  • The laser begins to oscillate only when the gain per round trip exceeds the loss; this requires a minimum pumping power, the threshold.
  • Above the threshold, the output grows quickly with pumping; below it the device behaves like a weak ordinary lamp (only spontaneous emission).
  • The mirrors reflecting 99.5 % and 98 % in the He-Ne laser keep the loss small, which is why a gas with small gain per pass can still lase.
  • A useful picture if the gain per pass is 3 % and the mirrors lose 2.5 % per round trip, the net growth is small but positive and the beam builds up over hundreds of passes until the gain falls to equal the loss (saturation).
  • This steady state gives the constant output power of a continuous laser.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 21 / 33
Continuous and pulsed operation

Continuous and pulsed operation

Comparison aspectMain ideaKeywords
Continuous-wave (CW) lasers
  • such as the He-Ne laser
  • give a steady beam of constant power (milliwatts to kilowatts)
givesteadybeamconstant
Pulsed lasers
  • such as the ruby laser pumped by a flash lamp
  • release the stored energy in short bursts (milliseconds down to femtoseconds). A short pulse has an enormous peak power even if its energy is small: 10 mJ in 10 ns is 1 MW. Femtosecond pulses (10−15 s) were used by Ahmed Zewail to follow the motion of atoms in a chemical reaction
  • like a camera with an extremely fast shutter
rubypumpedflashlamp
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 22 / 33
A guide to common lasers

A guide to common lasers

Laser Active medium Pumping Wavelength Typical use
Ruby chromium ions in an Al₂O₃ crystal flash lamp (optical) 694.3 nm (red) first laser; pulsed work
He-Ne He : Ne = 10 : 1 gas electric discharge 632.8 nm (red) alignment, scanners, teaching
Argon ion ionised argon gas electric discharge blue and green lines eye surgery, light shows
CO₂ molecular gas electric discharge 10.6 μm (infrared) industrial cutting and welding
Dye organic dye solution another laser tunable spectroscopy
Semiconductor p-n junction material electric current red / infrared CD players, pointers, optical fibres
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 23 / 33
Eye safety and classes

Eye safety and classes

  • A laser beam is collimated, so the lens of the eye focuses it on to a tiny spot of the retina, which can burn it.
  • For this reason never look directly into a laser beam or its reflection from a mirror; wear protective glasses suitable for the wavelength; low-power He-Ne or pointers are only safe if not stared at; infrared lasers are especially dangerous as they are invisible and the blink reflex does not protect the eye.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 24 / 33
Photon arithmetic for laser problems

Photon arithmetic for laser problems

  1. E = hc/λ (J) = 1240/λ(nm) (eV).
  2. Number of photons per second = power / energy of one photon.
  3. Number of photons in a pulse = pulse energy / energy of one photon.
  4. Peak power of a pulse = energy / pulse duration.
  5. Intensity of a beam = power / cross-sectional area.
  6. distance = c × (round-trip time)/2.
Comparison aspectMain ideaKeywords
Example 6.1.A 3 mW laser pointer emits green light of wavelength 532 nm. Photon energy = 1240/532 = 2.33 eV = 3.73 × 10−19 J. Photon rate = 3 × 10−3/3.73 × 10−19 = 8.0 × 1015 photons per secondlaserpointeremitsgreen
Example 6.2.
  • A pulsed ruby laser emits 0.5 J in 0.5 ms. Peak power = 0.5/5 × 10−4 = 1000 W. If this pulse is concentrated on an area of 1 mm2
  • the intensity is 1000/10−6 = 109 W/m2
  • which is enough to evaporate metal
pulsedrubylaseremits
Comparison aspectMain ideaKeywords
Example 6.3.
  • A laser beam leaves a source with diameter 2 mm and after 100 m its diameter is 2.4 mm. The intensity falls by (2/2.4)2 = 0.69
  • i.e. to 69 % of its initial value
  • whereas a point source would have fallen by a factor 104 at the same distance of 100 m compared with 1 m
laserbeamleavessource
Example 6.4.
  • An atom has an excited level at 2.30 eV above the ground level. It is stimulated to emit. Wavelength = 1240/2.30 = 539 nm (green)
  • and the output photon is in phase with the stimulating one
atomexcitedlevelabove
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 25 / 33
Typical exam questions and model answers (outline)

Typical exam questions and model answers (outline)

Comparison aspectMain ideaKeywords
Compare spontaneous and stimulated emissionuse the table of Lesson 1tableLesson
Explain the laser actionpopulation inversion → spontaneous photon along the axis → stimulated emission → multiple reflections → leak through the semitransparent mirrorpopulationinversionspontaneousphoton
Role of helium
  • it is easily excited by the discharge
  • its metastable levels are nearly equal to those of neon
  • so it transfers energy to neon by collisions and helps achieve population inversion
  • it is 10 times as abundant
easilyexciteddischargemetastable
Hologram versus photograph
  • the photograph records only intensity (2-D)
  • the hologram records amplitude and phase through interference with a reference beam
  • giving a 3-D image
recordsintensityamplitudephase
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 26 / 33
Chapter summary

Chapter summary

Comparison aspectMain ideaKeywords
•
  • LASER = Light Amplification by Stimulated Emission of Radiation. First laser: Maiman
  • 1960 (ruby)
LASERLightAmplificationStimulated
Spontaneous emission
  • random
  • incoherent
  • after the lifetime. Stimulated emission (Einstein
  • 1917): triggered by a photon of energy E₂ − E₁ before the lifetime ends
  • the new photon has the same frequency
  • phase and direction
randomincoherentafterlifetime
Laser properties
  • monochromatic
  • collimated
  • coherent
  • intense (not obeying the inverse-square law)
monochromaticcollimatedcoherentintense
Laser action needspopulation inversion → stimulated emission → amplification in the resonant cavitypopulationinversionstimulatedemission
Elements
  • active medium
  • pumping source
  • resonant cavity (one semitransparent mirror)
activemediumpumpingsource
He-Ne laser
  • He:Ne = 10:1 at 0.6 mm Hg
  • helium transfers energy to neon (nearly equal metastable levels)
  • output 632.8 nm
heliumtransfersenergyneon
Applications
  • holography
  • medicine
  • communications
  • industry
  • military
  • CDs
  • printers
  • shows
  • surveying
  • space research
holographymedicinecommunicationsindustry
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 27 / 33
Common mistakes

Common mistakes

  • Stimulated photons have the same phase, direction and frequency as the stimulating photon; the stimulating photon is not absorbed.
  • Population inversion is not the normal state; it is created by pumping through a metastable level.
  • In the He-Ne laser the lasing atoms are neon; helium only transfers energy.
  • A hologram needs coherent light and two beams (object and reference).
  • .egp-ex{margin:18px 0;border:1px solid rgba(79,63,224,.2);border-radius:16px;overflow:hidden;background:#fff}.egp-ex-h{padding:10px 16px;font-weight:800;background:linear-gradient(90deg,#4f3fe0,#22c1c3);color:#fff}.egp-ex-tabs{display:flex;flex-wrap:wrap;gap:6px;padding:10px 12px;background:#f7f6ff}.egp-ex-b{border:1px solid rgba(79,63,224,.3);background:#fff;border-radius:20px;padding:5px 14px;font-weight:700;cursor:pointer}.egp-ex-b.on{background:#4f3fe0;color:#fff}.egp-ex-p{padding:12px 16px}
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 28 / 33
Key Scientific Tables & Anatomical Diagrams Extracted from Official Curricula

Key Scientific Tables & Anatomical Diagrams Extracted from Official Curricula

💡 Core Diagrams & Reference Data→All data, reference comparison tables, and anatomical figures have been accurately digitized from official curriculum textbooks.

🔬 he_ne_laser_energy_levels_and_holography

  1. Scientific details and precise observational breakdown:
  2. ~. The accelerations of the two trains are equal.

a, =a

A B

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~ F=ma “=a om 27

B Mm «m

~ W=Fd

  • ‘. The two trains have covered the same distance in a straight line.
  • ~. The correct choice is (b).

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Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 29 / 33
Part 30

Part 30

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Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 30 / 33
📌 Comprehensive Scientific Terminology Dictionary:

📌 Comprehensive Scientific Terminology Dictionary:

  • LASER:
  • An acronym for "Light Amplification by Stimulated Emission of Radiation", producing highly monochromatic, coherent, collimated, and intense light beams.
  • Spontaneous Emission:
  • The transition of an excited atom to a lower energy state spontaneously without external influence after its lifetime expires (10-8 s), emitting a photon of random phase and direction.
  • Stimulated Emission:
  • The transition of an excited atom to a lower energy state triggered by an external incident photon whose energy matches the transition (hν = E2 – E1), emitting two identical, coherent photons in phase and direction.
  • Population Inversion:
  • A nonequilibrium thermodynamic condition where the number of atoms in a higher excited metastable state exceeds the number of atoms in the ground state.
  • Metastable State:
  • An excited atomic energy state with an exceptionally long lifetime (approximately 10-3 s, roughly $105$ times longer than ordinary levels), enabling accumulation of excited atoms.
  • ⚖️ Governing Scientific Laws, Theorems & Mathematical Models:
  • Stimulated Transition Condition:
  • [ Formula Incident photon energy: Ephoton = E2 – E1 striking an already excited atom before its natural lifetime ends. ]
  • Photon Multiplication Law:
  • [ Formula 1 incident photon + 1 excited atom → 2 coherent photons + 1 ground atom. (Amplification is exponential: 2 → 4 → 8 → 16 …). ]
  • Optical Resonator Condition:
  • [ Formula L = n λ / 2 (Cavity length must be an integral multiple of half-wavelengths to establish standing optical waves). ]
  • Holographic Interference Equation:
  • [ Formula Phase difference = 2π / λ × Path difference. (Holograms record both amplitude and phase). ]
  • 📌 Exhaustive In:
  • Depth Pedagogical Breakdown:
  • ◄ I. Spontaneous vs Stimulated Emission and Quantum Amplification
  • Ordinary light sources (such as tungsten bulbs, neon signs, and the Sun) operate predominantly via spontaneous emission.
  • Excited atoms return to lower levels randomly upon expiry of their brief lifetime ($10^{:
  • 8}$ s).
  • Consequently, emitted photons possess random phases, multiple wavelengths, and scatter in all spatial directions, losing intensity with distance according to the inverse-square law (I ∝ 1/d2).
  • In stimulated emission, predicted by Einstein in 1917, an atom in an excited state is struck by an external photon of exact resonant energy hν = E2: E1 BEFORE its lifetime expires.
  • The incident photon induces the atom to drop to the lower level, emitting a twin photon.
  • Both the incident and emitted photons emerge with identical energy, frequency, phase, polarization, and direction.
  • This stimulated emission process forms the fundamental mechanism of coherent optical amplification in lasers.
  • Figure (he_ne_laser_energy_levels_and_holography.png):
  • Figure (4) Energy level diagram of Helium and Neon and the optical setup for recording 3D holograms
  1. ◄ II. Three Core Pillars of a Functional Laser Generator
  2. Every laser device consists of three fundamental components:
  3. The Active Medium: The substance whose atoms or ions provide the laser transitions, existing as gases (He-Ne, CO2, Argon), liquids (organic dyes), or solids (Ruby, Nd:YAG, Semiconductor diodes).
  4. Pumping Energy Source: Provides external energy to excite atoms and achieve population inversion.
  5. Pumping methods include optical pumping (flash lamps or secondary lasers), electrical pumping (high-voltage DC discharge or radio frequencies), thermal pumping, and chemical pumping.
  6. Resonant Cavity: Consists of two parallel mirrors at the ends of the active medium—one fully reflecting (R ≈ 99.5%) and the other partially reflecting (R ≈ 98%).
  7. It forces photons to bounce back and forth through the active medium, triggering avalanche stimulated emissions and amplifying the light until a fraction escapes through the output coupler as an intense, parallel laser beam.
  • ◄ III. Operation of the Helium:

Neon Gas Laser (He-Ne)

  • The Helium:
  • Neon laser is a prominent continuous gas laser emitting visible red light at wavelength λ = 632.8 nm.
  • The active medium is a mixture of Helium and Neon gases in a 10:1 ratio at low pressure (0.6 mmHg) inside a quartz tube.
  • – Pumping Mechanism High-voltage DC discharge accelerates free electrons, which collide inelastically with Helium atoms, exciting them to the metastable level $E3$ (20.61 eV).
  • – Energy Transfer by Resonance Excited Helium atoms collide inelastically with ground-state Neon atoms. Because Neon possesses an energy level $E2$ (20.66 eV) remarkably close to Helium's $E3$, resonant energy transfer excites Neon atoms en masse, achieving Population Inversion in Neon.
  • – Laser Emission Excited Neon atoms transition from level $E2$ to level $E1$ via stimulated emission, radiating photons of wavelength 632.8 nm (red laser beam). The Neon atoms then quickly drop from $E1$ to the ground state via spontaneous emission, colliding with tube walls to release residual heat and readying themselves for the next cycle.
  • ◄ IV. Distinct Laser Characteristics and 3D Holography
  • Laser beams possess four unique properties:
  • 1. Monochromaticity: Extreme spectral purity with an ultra-narrow bandwidth (Δ λ ≈ 0).
  • 2. Coherence: Photons maintain constant phase relations over long distances and times.
  • 3. Collimation: Beam divergence is virtually zero; rays travel parallel without spreading.
  • 4. High Intensity: Energy is concentrated in a tiny cross-section, defying the inverse-square law.
  • Ordinary 2D photography records only light intensity (amplitude), losing all depth information.
  • In 1947, Dennis Gabor invented Holography (3D imaging).
  • A coherent laser beam is split into two:
  • an Object Beam (reflected from the 3D subject, carrying amplitude and phase/path differences) and a Reference Beam (reflected directly from a mirror).
  • The two beams interfere on a photographic plate, creating an interference pattern called a "Hologram".
  • When the developed hologram is illuminated with the same reference laser beam, the recorded wavefront reconstructs a fully parallax, floating 3D virtual image.
  • 🧮 Exemplary Step:
  • by-Step Worked Problems & Applied Exercises:
  • Worked Example 1:
  • Worked Problem 2 – Optical Resonance and Wavelength Calculation in He-Ne Laser
  • Problem Statement:
  • Problem A Helium-Neon laser emits a red laser beam of wavelength λ = 632.8 nm with an output power of 5 mW (5 × 10-3 W). Given h = 6.625 × 10-34 J·s and c = 3 × 108 m/s.
  • 1) Calculate the energy of a single laser photon in Joules and in electron-volts (eV).
  • 2) Calculate the number of photons emitted by the laser per second (N/t).
  • Detailed Solution:
  • 1) Photon energy E = hc / λ = (6.625 × 10-34 × 3 × 108) / (632.8 × 10-9) = (1.9875 × 10-25) / (632.8 × 10-9) ≈ 3.141 × 10-19 J.
  • In electron-volts EeV = (3.141 × 10-19) / (1.6 × 10-19) ≈ 1.963 eV.
  • 2) Number of photons emitted per second P = (N × E) / t ⇒ N / t = P / E = (5 × 10-3) / (3.141 × 10-19) ≈ 1.59 × 1016 photons/second.
  • 💡 Master Teacher Insights & Critical Exam Cautions:
  • Exam Secret:
  • In the He-Ne laser, the Helium atoms do NOT emit the laser beam!
  • Helium acts purely as an energy transfer intermediary; the NEON atoms are the active radiating species.
  • Metastable Lifetime:
  • Ordinary excited states last 10-8 s, whereas metastable states last 10-3 s—one hundred thousand times longer, allowing atoms to "pile up" for population inversion.
  • Holography Core:
  • To record a 3D hologram, the reference beam and object beam MUST originate from the SAME laser source to ensure mutual spatial and temporal coherence.
  • 🌍 Practical Real:
  • World, Industrial & Societal Connections:
  • ✔ Fiber:
  • Optic Telecommunications Semiconductor laser diodes transmit terabits of internet data per second across transoceanic fiber cables with minimal attenuation.
  • ✔ Medicine & Surgery:
  • Precision laser scalpels in eye surgeries (LASIK, retina detachment repair) and tumor ablations minimize bleeding by instantly cauterizing capillaries.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 31 / 33
🔍 In-Depth Explanations, Deductions & Multi-Book Insights:

🔍 In-Depth Explanations, Deductions & Multi-Book Insights:

  • ★ Comprehensive Study & Detailed Pedagogical Guide ★
  • Comprehensive Explanation Laser Physics, Spontaneous vs Stimulated Emission, Population Inversion, and the Helium-Neon Laser

| | 2026/2027 |

  • 🎯 Targeted Learning Outcomes & Pedagogical Objectives:
  • • Contrast spontaneous emission and stimulated emission in terms of photon phase, direction, and coherence.
  • • Explain the concepts of Population Inversion and Metastable Energy Levels.
  • • Identify the three essential components of any laser system (Active Medium, Pumping Energy Source, Resonant Cavity).
  • • Trace the operational sequence of the Helium-Neon Laser and analyze 3D holography principles.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 32 / 33
Lesson summary

Lesson summary

Comparison aspectMain ideaKeywords
•
  • ★ High-Yield Summary
  • Mind Maps & Comparison Tables ★
HighYieldSummaryMind
•🗺️ Core Concept Map & Knowledge ArchitectureCoreConceptKnowledgeArchitecture
✔ Emissions
  • Spontaneous (random
  • ordinary light) vs Stimulated (coherent twin photons
  • laser)
Spontaneousrandomordinarylight
✔ Laser PillarsActive Medium + Pumping Energy + Resonant Cavity (mirrors)ActiveMediumPumpingEnergy
✔ He-Ne LaserHe:Ne (10:1) | He excited by discharge | Resonant collision excites Ne | 632.8 nm red beamexciteddischargeResonantcollision
✔ Laser Qualities
  • Monochromaticity
  • Coherence
  • Collimation
  • High Intensity | 3D Holography
MonochromaticityCoherenceCollimationHigh
•📊 Classification & Comparative Summary TablesClassificationComparativeSummaryTables
TableComparison Between Spontaneous Emission and Stimulated EmissionComparisonBetweenSpontaneousEmission
Property Spontaneous Emission Stimulated Emission
Triggering Cause Internal atomic transition after natural lifetime expires External incident photon (hν = Δ E) striking excited atom
Lifetime in Upper Level Ordinary lifetime (10-8 seconds) Before lifetime expires (triggered prematurely)
Photon Multiplication 1 excited atom → 1 photon emitted 1 photon in + 1 atom → 2 coherent photons out
Coherence & Phase
  • Incoherent
  • completely random phase and polarization
  • Fully coherent
  • identical phase
  • direction
  • and polarization
Practical Examples
  • Sunlight
  • neon advertising tubes
  • incandescent lamps
  • He-Ne laser
  • Ruby laser
  • semiconductor laser diodes
  • 💡 Exam Flashcard Capsules & High-Yield Secrets:
  • ★ Laser intensity does not follow the Inverse Square Law because beam divergence is virtually zero.
  • ★ Metastable lifetime is 10-3 s, which is 100,000 times longer than ordinary lifetime (10-8 s).
  • ★ A hologram requires a coherent reference beam to reconstruct the 3D virtual image.
  • ★ Helium atoms return energy to ground state by colliding with the tube walls.
Lesson 1: Laser Physics, Population Inversion and the Helium-Neon Laser · 33 / 33