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Laser Linewidth and Coherence

Linewidth Δν and coherence length Lc = c/(πΔν) determine interferometry and spectroscopy performance. Narrow linewidth enables long-path interferometers; transform-limited pulses satisfy Δν×Δt ≥ TBP.

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Gaussian line shape: k ≈ 0.66; Lorentzian: k ≈ 0.32. Schawlow-Townes limit sets fundamental linewidth floor. Femtosecond pulses have THz bandwidth—broad spectral coverage. Single-frequency lasers achieve coherence lengths > 1 km.

Key quantities
0.54 mm
Coherence Length
Key relation
2.65 × 10^11 Hz
Linewidth
Key relation
1.81 × 10^-12 s
Coherence Time
Key relation
1064.00
Quality Factor
Key relation

Ready to run the numbers?

Why: Coherence length limits interferometer path difference and holography depth. Narrow linewidth enables precision spectroscopy. Transform-limited pulses maximize peak power for given bandwidth.

How: Lc = c/(π×Δν×k) with shape factor k. Time-bandwidth product Δν×Δt ≥ TBP (0.44 Gaussian). Cavity Δν = FSR/F from finesse.

Gaussian line shape: k ≈ 0.66; Lorentzian: k ≈ 0.32.Schawlow-Townes limit sets fundamental linewidth floor.

Run the calculator when you are ready.

Calculate Linewidth and CoherenceCoherence length, spectral bandwidth, cavity parameters

Spectral Parameters

laser-linewidth@bloomberg:~$
LINEWIDTH: BROAD
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Laser Linewidth Analysis
Linewidth: 2.65 × 10^11 Hz
Coherence Length: 0.54 mm • Quality Factor: 1.06e+3
numbervibe.com/calculators/physics/laser-linewidth-calculator

LINEWIDTH & COHERENCE ANALYSIS

Linewidth To Coherence

CALCULATED
LINEWIDTH (Δν)
2.65 × 10^11Hz
LINEWIDTH (Δλ)
1.0000nm
COHERENCE LENGTH
0.54mm
COHERENCE TIME
1.81 × 10^-12s
QUALITY FACTOR
1.06e+3
WAVENUMBER
9398.50 cm⁻¹
TL PULSE WIDTH
1.67 × 10^-12 s
PHOTON ENERGY
1.87 × 10^-19 J

📝 Calculation Steps

Step-by-Step Calculation
01

Input Parameters

02

Center Wavelength: 1064.00 nm

03

Center Frequency: 2.82 × 10^14 Hz

04

Linewidth to Coherence Conversion

05

Linewidth: 2.65 × 10^11 Hz

06

Linewidth: 1.0000 nm

07

Line Shape: gaussian (factor: 0.664)

08

Formula: Lc = c / (π × Δν × k)

ext{Lc} = c / (\text{pi} imes \text{Delta} ν imes k)

09

Coherence Length: 0.54 mm→ 0.54 mm

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Coherence Time: 1.81 × 10^-12 s

11

Quality Metrics

12

Quality Factor (Q): 1.06e+3

13

Spectral Purity: 9.40 × 10^-4

Visualizations

For educational and informational purposes only. Verify with a qualified professional.

🔬 Physics Facts

📐

Coherence length limits maximum path difference in Michelson interferometers.

— RP Photonics

Schawlow-Townes limit sets quantum minimum linewidth for laser oscillators.

— NIST

🔬

Transform-limited pulses have minimum bandwidth for given duration.

— Ultrafast Optics

📡

Fiber lasers can achieve sub-kHz linewidth for metrology applications.

— Thorlabs

📋 Key Takeaways

  • • Laser linewidth (Δν or Δλ) is the spectral width measured as full-width at half-maximum (FWHM) and determines coherence properties
  • • Coherence length is inversely proportional to linewidth: Lc = c / (π × Δν) for Lorentzian lineshapes
  • • Narrower linewidth enables longer coherence lengths, essential for interferometry, LIDAR, and fiber sensing applications
  • • The time-bandwidth product (TBP) sets the minimum bandwidth for transform-limited pulses: Δν × Δt ≥ TBP
  • • Single-frequency lasers achieve sub-kHz linewidths with coherence lengths exceeding kilometers

🤔 Did You Know?

The Schawlow-Townes limit sets the fundamental quantum limit on laser linewidth, but real lasers typically operate 10-100× above this limit due to technical noise sources.

Source: Schawlow & Townes (1958), Physical Review

Frequency-stabilized HeNe lasers can achieve linewidths below 1 MHz, enabling coherence lengths over 100 meters for precision metrology applications.

Source: NIST Laser Metrology Standards

Ultra-narrow linewidth fiber lasers (<100 Hz) enable distributed fiber sensing over distances exceeding 100 km, revolutionizing structural health monitoring.

Source: OSA/Optica Photonics Technology Letters

💡 Expert Tips

  • • For interferometry applications, ensure coherence length exceeds the maximum optical path difference by at least 3×
  • • Use Pound-Drever-Hall locking or frequency offset locking to stabilize laser frequency and reduce linewidth
  • • Higher cavity finesse and longer cavity length reduce linewidth according to Δν = FSR / F
  • • Consider line shape (Gaussian vs Lorentzian) when calculating coherence length, as shape factors differ significantly
  • • For transform-limited pulses, choose pulse shape carefully—Gaussian pulses have TBP = 0.441, while sech² pulses have TBP = 0.315

Laser linewidth (Δν or Δλ) is the spectral width of the laser emission, typically measured as the full-width at half-maximum (FWHM). It's inversely related to coherence length—narrower linewidth means longer coherence and better interferometric performance.

Key Relationships

Lc = c / (π × Δν)

Coherence length

Δν × Δt ≥ TBP

Time-bandwidth product

Typical Laser Linewidths

Laser TypeLinewidthCoherence LengthApplications
Stabilized HeNe<1 MHz>100 mMetrology, interferometry
Single-freq Nd:YAG1-100 kHz1-100 kmLIDAR, holography
DFB Fiber Laser1-100 kHz1-100 kmFiber sensing
ECDL (External Cavity)100 kHz-1 MHz100 m-3 kmSpectroscopy
Multi-mode diode1-3 nm0.1-0.3 mmPumping, illumination
Femtosecond Ti:Sapph10-100 nm3-30 μmUltrafast spectroscopy

Time-Bandwidth Product

The time-bandwidth product (TBP) is the minimum product of pulse duration and spectral bandwidth, set by the Fourier transform relationship. Different pulse shapes have different TBP constants.

Gaussian

0.441

Sech²

0.315

Lorentzian

0.142

Rectangular

0.886

Coherence Requirements for Applications

ApplicationMin. Coherence LengthMax. LinewidthNotes
Fiber Gyroscope>1 km<100 kHzLong fiber coil
LIDAR (long range)>100 m<1 MHzCoherent detection
Holography>1 m<100 MHzScene depth dependent
Surface Profilometry>1 cm<10 GHzOptical path difference
Fiber Sensing>10 m<10 MHzDistributed sensing

Linewidth Unit Conversions

Converting between frequency, wavelength, and wavenumber linewidths at center wavelength λ₀:

Δν ↔ Δλ

Δλ = (λ₀² / c) × Δν

Δν ↔ Δσ

Δσ = Δν / c (cm⁻¹)

Δλ ↔ Δσ

Δσ = Δλ / λ₀² (cm⁻¹)

❓ Frequently Asked Questions

Q: What is the difference between linewidth and bandwidth?

Linewidth typically refers to the spectral width of a continuous-wave laser, while bandwidth often describes the frequency spread of pulsed lasers. Both measure spectral spread but in different contexts.

Q: How does linewidth affect interferometry?

Narrower linewidth provides longer coherence length, allowing larger optical path differences before interference fringes disappear. For stable interference, coherence length should exceed the path difference by 3-5×.

Q: What causes laser linewidth broadening?

Technical noise (vibrations, temperature fluctuations, current noise), quantum noise (Schawlow-Townes limit), and cavity losses all contribute. Frequency stabilization techniques can reduce technical noise significantly.

Q: Can I measure linewidth directly?

Yes, using techniques like self-heterodyne detection, Fabry-Perot interferometry, or delayed self-heterodyne. For very narrow linewidths (<1 MHz), specialized equipment is required.

Q: What is the relationship between finesse and linewidth?

Higher cavity finesse (F) narrows the linewidth: Δν = FSR / F, where FSR is the free spectral range. This is why high-finesse cavities enable ultra-narrow linewidth lasers.

Q: How do I choose the right linewidth for my application?

Match coherence length to your application: LIDAR needs >100 m (linewidth <1 MHz), interferometry needs >1 m (<100 MHz), while pumping applications can tolerate much broader linewidths (>1 nm).

Q: What is transform-limited bandwidth?

The minimum spectral bandwidth for a given pulse duration, set by the Fourier transform relationship. Transform-limited pulses have the shortest duration possible for their bandwidth, with no excess chirp.

⚠️ Disclaimer: This calculator provides theoretical estimates for educational purposes only. Actual laser linewidth depends on many factors including cavity design, stabilization techniques, environmental conditions, and technical noise sources. For precision applications, consult laser manufacturers and use calibrated measurement equipment. Always follow laser safety guidelines and regulations.

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