Chapter 11: Laser Mirrors and Regenerative Feedback =================================================== Source: Anthony E. Siegman, *Lasers* (1986), Chapter 11. Use each section/problem identifier with the book; the original prompts are not reproduced here. Each entry gives the governing model, the decisive solution route, and a physical verification. Section 11.1: Laser Mirrors And Beam Splitters ---------------------------------------------- Problem 11.1.1 — Scattering matrix for a general dielectric slab ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.1.2 — Changes in the scattering matrix for different reference planes ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.1.3 — Derivation of the necessary matrix element relationships for a lossless reciprocal two-port ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ Begin with the stated physical law, keep the derivation symbolic, and introduce each approximation only where its limiting condition is explicit. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.1.4 — Scattering matrix for a transmission line junction ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.1.5 — Transmission-line junction with a lumped shunt capacitance ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.1.6 — Three-port and five-port optical scattering systems? ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.1.7 — Impossibility of a completely matched three-port network ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.1.8 — Conditions for an N-port equal-amplitude beam splitter ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.1.9 — Synthesizing an arbitrary complex optical two-port (research problem) ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ Normalize the variables first, evaluate the analytic limits, and then sweep the remaining dimensionless parameter so the numerical curve can be checked against both limits. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Section 11.3: Resonance Properties Of Passive Optical Cavities -------------------------------------------------------------- Problem 11.3.1 — Design specifications for a transmission etalon ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ Translate each performance requirement into an equality or inequality, solve the coupled constraints, and discard any root that violates a physical bound. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.3.2 — Angle tuning of a transmission etalon ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.3.3 — Calculating cavity parameters from measured transmission-reflection curves ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.3.4 — Reflection properties of uncoated dielectric etalon mirrors ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.3.5 — Linewidth of a power reflectivity dip ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.3.6 — Reflection phase angle versus frequency ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ Evaluate both cases from the same symbolic expression before taking their ratio; this keeps normalization and sign conventions from obscuring the comparison. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.3.7 — Field magnification inside a resonant cavity ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Section 11.5: Optical-Cavity Mode Frequencies --------------------------------------------- Problem 11.5.1 — Axial-mode spectrum for an optical cavity with an internal dielectric section ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.5.2 — Axial-mode spectrum including dispersion ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Expand :math:`k(\omega)` about the carrier, retain the requested orders, and use :math:`v_g=(dk/d\omega)^{-1}` with :math:`k''` controlling quadratic dispersive broadening. Check the transform-limited and zero-dispersion limits, and conserve pulse energy when only phase is changed. Problem 11.5.3 — Resonance properties of an equilateral triangular dielectric prism ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.5.4 — Mirror spacing in an optically pumped thin dye laser ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Section 11.6: Regenerative Laser Amplification ---------------------------------------------- Problem 11.6.1 — Reflection gain of a regenerative laser amplifier ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Propagate irradiance with :math:`dI/dz=g(I)I`, using :math:`g(I)=g_0/(1+I/I_s)` when saturation matters; integrate before inserting boundary values. Verify that the small-signal limit is exponential, while extracted energy never exceeds the stored inversion energy. Problem 11.6.2 — Phase angle versus frequency for a regenerative laser cavity amplifier ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ Evaluate both cases from the same symbolic expression before taking their ratio; this keeps normalization and sign conventions from obscuring the comparison. Propagate irradiance with :math:`dI/dz=g(I)I`, using :math:`g(I)=g_0/(1+I/I_s)` when saturation matters; integrate before inserting boundary values. Verify that the small-signal limit is exponential, while extracted energy never exceeds the stored inversion energy. Problem 11.6.3 — Enhanced feedback diagram ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Propagate irradiance with :math:`dI/dz=g(I)I`, using :math:`g(I)=g_0/(1+I/I_s)` when saturation matters; integrate before inserting boundary values. Verify that the small-signal limit is exponential, while extracted energy never exceeds the stored inversion energy. Section 11.7: Approaching Threshold: The Highly Regenerative Limit ------------------------------------------------------------------ Problem 11.7.1 — Power transmission through a laser cavity halfway between axial modes ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.7.2 — Gain sensitivity of a regenerative laser amplifier ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Propagate irradiance with :math:`dI/dz=g(I)I`, using :math:`g(I)=g_0/(1+I/I_s)` when saturation matters; integrate before inserting boundary values. Verify that the small-signal limit is exponential, while extracted energy never exceeds the stored inversion energy. Problem 11.7.3 — Skirt selectivity of a regenerative laser amplifier ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Propagate irradiance with :math:`dI/dz=g(I)I`, using :math:`g(I)=g_0/(1+I/I_s)` when saturation matters; integrate before inserting boundary values. Verify that the small-signal limit is exponential, while extracted energy never exceeds the stored inversion energy. Problem 11.7.4 — Output versus input for a regenerative laser amplifier with saturable internal gain ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ Evaluate both cases from the same symbolic expression before taking their ratio; this keeps normalization and sign conventions from obscuring the comparison. Propagate irradiance with :math:`dI/dz=g(I)I`, using :math:`g(I)=g_0/(1+I/I_s)` when saturation matters; integrate before inserting boundary values. Verify that the small-signal limit is exponential, while extracted energy never exceeds the stored inversion energy. Problem 11.7.5 — Regenerative gain peaks for off-line-center axial modes ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Propagate irradiance with :math:`dI/dz=g(I)I`, using :math:`g(I)=g_0/(1+I/I_s)` when saturation matters; integrate before inserting boundary values. Verify that the small-signal limit is exponential, while extracted energy never exceeds the stored inversion energy. Problem 11.7.6 — Transient reflection from a resonant cavity ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold. Problem 11.7.7 — Approach to threshold in the Schawlow-Townes model ^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^ List the supplied quantities in one unit system, isolate the requested variable symbolically, and retain guard digits until the final evaluation. Form the complex round-trip factor :math:`G_{rt}=|G_{rt}|e^{j\Phi}`; resonance requires :math:`\Phi=2\pi q`, and threshold requires :math:`|G_{rt}|=1`. Check the passive-cavity limit, energy conservation at every mirror, and that added loss raises rather than lowers threshold.