{"id":2376,"date":"2026-09-01T09:05:35","date_gmt":"2026-09-01T09:05:35","guid":{"rendered":"https:\/\/photo-detector.com\/?p=2376"},"modified":"2026-09-01T09:05:41","modified_gmt":"2026-09-01T09:05:41","slug":"retroalimentacion-de-bucle-cerrado-del-escaner-de-galvano","status":"publish","type":"post","link":"https:\/\/photo-detector.com\/es\/galvanometer-scanner-closed-loop-feedback\/","title":{"rendered":"Dise\u00f1o de circuitos de realimentaci\u00f3n en lazo cerrado para esc\u00e1neres galvo: del fotodiodo al control PID"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">If you have ever wrestled with a high-speed laser marking head drifting off-target by 200 microradians halfway through an eight-hour shift, you already know the culprit. It is almost never the digital coordinate generator or the laser source itself. The headache lives directly inside the analog-to-digital sensor chain and the servo driver circuitry.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Building a rock-solid <strong>galvanometer scanner closed loop feedback<\/strong> circuit means turning microamps of optical current into sub-microradian positional accuracy under brutal mechanical acceleration. Galvo rotors whip back and forth at 2 kHz to 5 kHz, generating back-EMF, thermal spikes, and high-frequency noise that loves nothing more than corrupting your sensor traces.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">When we evaluate a modern <strong>galvanometer scanner closed loop feedback<\/strong> architecture, we are looking at an integrated physical and digital signal chain:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>The Galvanometer Feedback Signal Chain:<\/strong><br><strong>1. Optical Source &amp; Modulation:<\/strong> Infrared LED or VCSEL emitting stable optical flux across an internal rotor paddle.<br><strong>2. Optical Transduction:<\/strong> Balanced Silicon PIN photodiodes capturing differential light flux proportional to angular rotor position.<br><strong>3. Analog Front-End (TIA):<\/strong> Low-noise transimpedance amplifiers converting nanoamps and microamps into high-level voltage signals.<br><strong>4. Normalization Stage:<\/strong> Sum-and-difference ratiometric division circuit to eliminate emitter intensity fluctuations and thermal drift.<br><strong>5. Signal Acquisition:<\/strong> High-speed, zero-latency Successive Approximation Register (SAR) ADC conversion.<br><strong>6. Digital Servo Processing:<\/strong> DSP or FPGA running high-rate discrete PID calculation, velocity\/acceleration feedforward, and mechanical resonance notch filtering.<br><strong>7. Current Output Stage:<\/strong> Transconductance power amplifier driving the galvo rotor voice coil with controlled torque.<\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">Let&#8217;s walk through the entire physical feedback loop step by step: from the physical silicon photodiode receiving optical flux behind the moving vane, through transimpedance amplification, error conditioning, ADC quantization, and down to the PID and notch filter algorithms running on your digital signal processor.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">The Physics of the Optical Position Detector (PD Inside the Galvo)<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">Inside an optical closed-loop galvanometer scanner, angular position is measured using an optical blocking vane attached directly to the rear of the rotor shaft. An infrared emitter (LED or VCSEL) shines light across this vane onto a balanced pair of Silicon PIN photodiodes or a segmented quadrant detector.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">As the rotor turns, the vane selectively shadows one photodiode while exposing more active area on the other. This mechanical differential shuttering creates two complementary photocurrents, Ia and Ib.<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Key Rule of Galvo Optical Sensors:<\/strong> Never rely on absolute single-ended photodiode current. Any fluctuation in emitter output due to temperature will register as false mechanical displacement. You must always use a differential, ratiometric measurement scheme:<br><strong>Position Output = (Ia &#8211; Ib) \/ (Ia + Ib)<\/strong><\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">By dividing the differential photocurrent (Ia &#8211; Ib) by the total photocurrent (Ia + Ib), the <strong>galvanometer scanner closed loop feedback<\/strong> mathematically cancels out LED aging, emitter drive ripple, and ambient thermal drift.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">Front-End Sensor Selection: Silicon PIN Photodiodes for Galvo Systems<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">Your choice of front-end photodetector dictates the noise floor, bandwidth, and long-term thermal stability of the entire <strong>galvanometer scanner closed loop feedback<\/strong> loop.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">For high-speed laser scan heads, you need PIN photodiodes characterized by low junction capacitance (Cj &lt; 15 pF at reverse bias), ultra-low dark current (Id &lt; 1 nA at 25\u00b0C), and matched spectral responsivity in the near-infrared band (typically 850 nm to 940 nm).<\/p>\n\n\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><thead><tr><th>Parameter<\/th><th>BeePhoton PDC-C2928-NIR-B<\/th><th>BeePhoton PDC-C2929<\/th><th>BeePhoton PDC-2C3432-NIR-B<\/th><\/tr><\/thead><tbody><tr><td><strong>Detector Architecture<\/strong><\/td><td>Single PIN Die<\/td><td>High-Speed PIN Die<\/td><td>Dual-Segment Dual PIN Die<\/td><\/tr><tr><td><strong>Peak Responsivity<\/strong><\/td><td>940 nm<\/td><td>920 nm<\/td><td>940 nm<\/td><\/tr><tr><td><strong>Junction Capacitance (Cj)<\/strong><\/td><td>8.5 pF @ 5V<\/td><td>6.2 pF @ 5V<\/td><td>12.0 pF per element @ 5V<\/td><\/tr><tr><td><strong>Dark Current (Id)<\/strong><\/td><td>0.25 nA @ -5V<\/td><td>0.18 nA @ -5V<\/td><td>0.50 nA @ -5V<\/td><\/tr><tr><td><strong>Rise Time (tr)<\/strong><\/td><td>4.5 ns<\/td><td>3.2 ns<\/td><td>6.0 ns<\/td><\/tr><tr><td><strong>Active Area Geometry<\/strong><\/td><td>Matched Single Pad<\/td><td>Ultra-Compact Pad<\/td><td>Monolithic Dual Strip<\/td><\/tr><tr><td><strong>Primary Galvo Role<\/strong><\/td><td>Compact Scan Heads<\/td><td>Ultra-High Speed Scanners<\/td><td>Balanced Differential Feedback<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"wp-block-paragraph\">When designing high-bandwidth feedback loops, we frequently utilize matched sensor dies. For classic balanced paddle architectures, the <strong><a href=\"https:\/\/photo-detector.com\/product\/segmented-pin-photodiode-chip\/\" target=\"_blank\" rel=\"noreferrer noopener\">PDC-2C3432-NIR-B segmented PIN photodiode chip<\/a><\/strong> provides near-identical thermal tracking across both channels because both active areas share the exact same monolithic silicon substrate.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">If your design demands independent physical placement on opposite sides of a cylindrical rotor shaft, utilizing discrete, low-capacitance chips like the <strong><a href=\"https:\/\/photo-detector.com\/product\/940nm-pin-photodiode-chip\/\" target=\"_blank\" rel=\"noreferrer noopener\">PDC-C2928-NIR-B 940nm photodiode<\/a><\/strong> or the ultra-low dark current <strong><a href=\"https:\/\/photo-detector.com\/product\/920nm-silicon-pin-photodiode\/\" target=\"_blank\" rel=\"noreferrer noopener\">PDC-C2929 920nm silicon PIN photodiode<\/a><\/strong> allows precision mechanical alignment while keeping front-end capacitance low enough to preserve phase margin in your <strong>galvanometer scanner closed loop feedback<\/strong>.<\/p>\n\n\n\n<div data-block-name=\"woocommerce\/single-product\" data-product-id=\"2234\" data-wp-context=\"woocommerce\/products::{&quot;productId&quot;:2234,&quot;variationId&quot;:null}\" data-wp-interactive=\"woocommerce\/single-product\" class=\"wp-block-woocommerce-single-product woocommerce\">\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-7387b849 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<div data-block-name=\"woocommerce\/product-gallery\" 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wp-block-woocommerce-product-gallery-is-layout-flex\">\n\n\t\t\t<div data-block-name=\"woocommerce\/product-gallery-large-image\" class=\"wc-block-product-gallery-large-image wp-block-woocommerce-product-gallery-large-image\">\n\t\t\t\t\t\t\t\t\t\t\t<ul\n\t\t\t\tclass=\"wc-block-product-gallery-large-image__container\"\n\t\t\t\tdata-wp-interactive=\"woocommerce\/product-gallery\"\n\t\t\t\tdata-wp-on--keydown=\"actions.onViewerImageKeyDown\"\n\t\t\t\taria-label=\"Galer\u00eda del producto\"\n\t\t\t\ttabindex=\"0\"\n\t\t\t\taria-roledescription=\"carousel\"\n\t\t\t>\n\t\t\t\t\t\t\t\t\t<li\n\t\t\t\t\t\tclass=\"wc-block-product-gallery-large-image__wrapper\"\n\t\t\t\t\t>\n\t\t\t\t\t\t<div data-block-name=\"woocommerce\/product-image\" data-is-descendent-of-single-product-block=\"true\" data-show-product-link=\"false\" data-show-sale-badge=\"false\" class=\"wc-block-components-product-image wc-block-grid__product-image wc-block-components-product-image--aspect-ratio-auto wp-block-woocommerce-product-image\"><img fetchpriority=\"high\" decoding=\"async\" data-wp-on--click=\"actions.openDialog\" data-wp-on--mouseleave=\"actions.resetZoom\" data-wp-on--mousemove=\"actions.startZoom\" data-wp-on--touchend=\"actions.onTouchEnd\" data-wp-on--touchmove=\"actions.onTouchMove\" data-wp-on--touchstart=\"actions.onTouchStart\" data-wp-watch=\"callbacks.toggleImageVisibility\" draggable=\"false\" fetchpriority=\"high\" tabindex=\"-1\" width=\"800\" height=\"800\" src=\"https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-1024x1024.webp\" class=\"attachment-large size-large wc-block-woocommerce-product-gallery-large-image__image wc-block-woocommerce-product-gallery-large-image__image--full-screen-on-click wc-block-woocommerce-product-gallery-large-image__image--hoverZoom\" alt=\"PDC-C2929 cost effective 920nm silicon PIN photodiode chip for laser scanner\" data-testid=\"product-image\" data-image-id=\"2235\" style=\"object-fit:cover;\" 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height=\"24\" aria-hidden=\"true\" focusable=\"false\">\n\t\t\t\t\t\t\t<path d=\"M13 11.8l6.1-6.3-1-1-6.1 6.2-6.1-6.2-1 1 6.1 6.3-6.5 6.7 1 1 6.5-6.6 6.5 6.6 1-1z\"><\/path>\n\t\t\t\t\t\t<\/svg>\n\t\t\t\t\t<\/button>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"wc-block-product-gallery-dialog__content\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img\n\t\t\t\t\t\t\t\tdata-image-id=\"2235\"\n\t\t\t\t\t\t\t\tdata-wp-watch=\"callbacks.toggleImageVisibility\"\n\t\t\t\t\t\t\t\tsrc=\"https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-scaled.webp\"\n\t\t\t\t\t\t\t\tsrcset=\"https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-scaled.webp 2560w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-300x300.webp 300w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-1024x1024.webp 1024w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-150x150.webp 150w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-768x768.webp 768w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-1536x1536.webp 1536w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-2048x2048.webp 2048w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-12x12.webp 12w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-600x600.webp 600w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2929-100x100.webp 100w\"\n\t\t\t\t\t\t\t\tsizes=\"(max-width: 2560px) 100vw, 2560px\"\n\t\t\t\t\t\t\t\tdecoding=\"async\"\n\t\t\t\t\t\t\t\talt=\"PDC-C2929 cost effective 920nm silicon PIN photodiode chip for laser scanner\" \/>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t<\/dialog>\n\t\t<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\"><h2 class=\"wp-block-post-title\"><a href=\"https:\/\/photo-detector.com\/es\/product\/920nm-silicon-pin-photodiode\/\" target=\"_blank\" >Si PIN photodiodes for Galvo PDC-C2929<\/a><\/h2>\n\n<div data-block-name=\"woocommerce\/product-summary\" data-is-descendent-of-single-product-block=\"true\" class=\"wp-block-woocommerce-product-summary\"><div class=\"wc-block-components-product-summary \" style=\"\">\n\t\t\t\t<p>The PDC-C2929 is a budget-friendly 920nm silicon PIN photodiode chip. This 920nm silicon PIN photodiode offers stable, cost-effective scanner position tracking.<\/p>\n\n\t\t\t<\/div><\/div>\n\n\n<div data-block-name=\"woocommerce\/product-meta\" class=\"wp-block-woocommerce-product-meta\">\n<div class=\"wp-block-group is-nowrap is-layout-flex wp-container-core-group-is-layout-7387b849 wp-block-group-is-layout-flex\">\n\n<div class=\"taxonomy-product_tag wp-block-post-terms\"><span class=\"wp-block-post-terms__prefix\">Tag\uff1a<\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/920nm-pin-photodiode\/\" rel=\"tag\">920nm PIN Photodiode<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/bee-photon\/\" rel=\"tag\">Bee Photon<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/budget-photodiode-chip\/\" rel=\"tag\">Budget Photodiode Chip<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/galvo-sensor\/\" rel=\"tag\">Galvo Sensor<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/silicon-pin-photodiode\/\" rel=\"tag\">Silicon PIN photodiode<\/a><\/div><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">Front-End TIA Design: Turning Microamps into Stable Voltage<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">The transimpedance amplifier (TIA) converts the photodiode current (typically 10 uA to 500 uA full-scale) into a usable analog voltage. In a <strong>galvanometer scanner closed loop feedback<\/strong> circuit, this stage is where phase margin goes to die if layout parasitics and capacitance compensation are neglected.<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Operational Amplifier TIA Topology:<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>Photodiode anode\/cathode connects directly to the inverting input of an ultra-low input bias current op-amp (JFET or CMOS input, e.g., OPA656 or ADA4817).<\/li>\n\n\n\n<li>Feedback resistor Rf is tied between the op-amp output and the inverting input.<\/li>\n\n\n\n<li>Feedback compensation capacitor Cf is tied in parallel with Rf to cancel the high-frequency pole caused by sensor junction capacitance.<\/li>\n\n\n\n<li>Non-inverting terminal connects to clean analog ground or a precision low-noise reference bias.<\/li>\n<\/ul>\n<\/blockquote>\n\n\n\n<h3 class=\"wp-block-heading\">1. Transimpedance Gain and Output Voltage Calculation<\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">For each photodiode channel, the output voltage is given by the simple gain relationship:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Vout = -Ipd * Rf<\/strong><\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">Where:<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Ipd<\/strong> = Photocurrent generated by the sensor under NIR illumination (Amperes)<\/li>\n\n\n\n<li><strong>Rf<\/strong> = Transimpedance feedback resistor value (Ohms)<\/li>\n<\/ul>\n\n\n\n<p class=\"wp-block-paragraph\">If your maximum photodiode current is 250 uA and your target ADC driver headroom is 2.5 V, select:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Rf = 2.5 V \/ 250 uA = 10,000 Ohms (10 kOhm)<\/strong><\/p>\n<\/blockquote>\n\n\n\n<h3 class=\"wp-block-heading\">2. Feedback Capacitance (Cf) for Stability and Phase Margin<\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">The total input capacitance Cin looking into the inverting terminal is the sum of all parallel capacitances:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Cin = Cj (Photodiode Junction Cap) + Ccm (Op-Amp Common Mode Cap) + Cdiff (Op-Amp Diff Cap) + Ctrace (PCB Parasitics)<\/strong><\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">Without a feedback capacitor Cf across Rf, the pole formed by Rf and Cin creates an uncompensated phase lag, causing ringing, overshoot, or outright oscillation in your position feedback. To achieve a maximally flat Butterworth response (45 to 60 degrees of phase margin), calculate Cf using the standard <strong><a href=\"https:\/\/www.ti.com\/lit\/an\/sboa122\/sboa122.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">Texas Instruments Transimpedance Stability Formulation<\/a><\/strong>:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Cf = sqrt( Cin \/ ( 2 * pi * Rf * GBW ) )<\/strong><\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">Where <strong>GBW<\/strong> is the Gain-Bandwidth Product of your operational amplifier.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Let&#8217;s calculate real values for an actual high-speed <strong>galvanometer scanner closed loop feedback<\/strong> circuit:<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>Cin = 15 pF (Photodiode Cj + stray PCB capacitance)<\/li>\n\n\n\n<li>Rf = 20 kOhm<\/li>\n\n\n\n<li>Op-Amp = OPA656 (GBW = 230 MHz)<\/li>\n<\/ul>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Step 1:<\/strong> Calculate Denominator: 2 * 3.14159 * 20000 * 230,000,000 = 2.8902e13<br><strong>Step 2:<\/strong> Divide Cin by Denominator: 15e-12 \/ 2.8902e13 = 5.1899e-25<br><strong>Step 3:<\/strong> Take Square Root: sqrt( 5.1899e-25 ) \u2248 0.72 pF<\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">In practice, place a 0.8 pF to 1.0 pF ultra-stable C0G\/NP0 ceramic capacitor across Rf. If you omit this, your scan head servo will likely buzz, develop limit-cycle oscillations, or experience high-frequency tracking jitter.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">3. TIA Noise Floor and Johnson Noise<\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">The feedback resistor generates thermal Johnson-Nyquist noise:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Vn_res = sqrt( 4 * kB * T * Rf * Delta_f )<\/strong><\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">Where:<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>kB<\/strong> = 1.380649e-23 J\/K (Boltzmann&#8217;s constant)<\/li>\n\n\n\n<li><strong>T<\/strong> = Absolute temperature in Kelvin (e.g., 300 K)<\/li>\n\n\n\n<li><strong>Delta_f<\/strong> = Feedback circuit noise bandwidth<\/li>\n<\/ul>\n\n\n\n<p class=\"wp-block-paragraph\">Keep Rf as small as practical while maintaining adequate signal-to-noise ratio (SNR) so that input voltage noise from the operational amplifier does not dominate when multiplied by the noise gain at high frequencies in your <strong>galvanometer scanner closed loop feedback<\/strong> front-end.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">Signal Conditioning: The Ratiometric Sum-and-Difference Engine<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">Once you have converted channel A and channel B currents into voltages (Va and Vb), you must execute the differential and sum operations before digitizing.<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Dual-Channel Processing Paths:<\/strong><br><strong>Difference Channel Output:<\/strong> Vdiff = (Va &#8211; Vb) -&gt; Represents instantaneous angular shaft displacement.<br><strong>Sum Channel Output:<\/strong> Vsum = (Va + Vb) -&gt; Represents total received light flux for dynamic AGC or normalization.<\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">In high-end analog galvo drivers, the sum channel is fed into an Automatic Gain Control (AGC) circuit or an analog divider IC. In modern DSP-driven digital servo controllers, both the difference and sum channels are digitized directly, or Va and Vb are sampled simultaneously using a multi-channel synchronous ADC, allowing the processor to perform the ratiometric normalization:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Normalized_Position = ( Va &#8211; Vb ) \/ ( Va + Vb )<\/strong><\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">This digital division completely immunizes your <strong>galvanometer scanner closed loop feedback<\/strong> against emitter thermal degradation over thousands of operational hours.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">ADC Selection and Anti-Aliasing Filter Design<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">In modern digital galvo servo drivers, your PID loop update rate is typically between 100 kHz and 500 kHz. Any phase delay introduced by the ADC or its anti-aliasing filter directly eats into your loop&#8217;s phase margin.<\/p>\n\n\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><thead><tr><th>Specification Parameter<\/th><th>Traditional Analog Servo Driver<\/th><th>Modern Digital DSP Servo Controller<\/th><\/tr><\/thead><tbody><tr><td><strong>Position Resolution<\/strong><\/td><td>Continuous (Thermal Noise Limited)<\/td><td>16-bit to 18-bit True No-Missing-Codes<\/td><\/tr><tr><td><strong>Feedback Loop Bandwidth<\/strong><\/td><td>2.5 kHz to 4.0 kHz<\/td><td>3.5 kHz to 6.5 kHz<\/td><\/tr><tr><td><strong>Drift Compensation<\/strong><\/td><td>Manual Trimpots &amp; NTC Thermistors<\/td><td>Dynamic Polynomial Digital Look-Up Table<\/td><\/tr><tr><td><strong>Notch Filter Tuning<\/strong><\/td><td>Fixed Twin-T \/ Sallen-Key Op-Amps<\/td><td>Dynamic Multi-Notch Digital IIR Cascades<\/td><\/tr><tr><td><strong>Commutation &amp; Calibration<\/strong><\/td><td>Dual-Trace Scope &amp; Pot Tweaking<\/td><td>Software GUI Step-Response Auto-Tuning<\/td><\/tr><tr><td><strong>Noise Susceptibility<\/strong><\/td><td>High (Long Analog Control Traces)<\/td><td>Low (Direct Localized ADC Digitization)<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<h3 class=\"wp-block-heading\">1. Anti-Aliasing Filter (AAF)<\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Do not use high-order active filters with steep roll-offs (like a 4th-order Chebyshev) right before your ADC. While they attenuate out-of-band noise effectively, their severe group delay will ruin the phase margin of your <strong>galvanometer scanner closed loop feedback<\/strong> loop.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Instead, implement a balanced 2nd-order active Sallen-Key or Multiple-Feedback (MFB) Bessel filter, or even a simple 1st-order differential RC filter if your ADC sampling rate is sufficiently high (e.g., 2 MSPS SAR ADC oversampled).<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">The -3 dB cutoff frequency is typically set to 3 to 5 times the closed-loop servo bandwidth:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>fc = 1 \/ ( 2 * pi * R * C * sqrt(2) )<\/strong><\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">For a 50 kHz anti-aliasing cutoff:<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>Select R = 499 Ohms (0.1% tolerance thin-film resistor)<\/li>\n\n\n\n<li>Calculate C \u2248 4.5 nF (Use standard 4.7 nF C0G capacitor)<\/li>\n<\/ul>\n\n\n\n<h3 class=\"wp-block-heading\">2. ADC Selection<\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">Use a Successive Approximation Register (SAR) ADC with zero conversion latency, such as the AD4003 or ADS8881 (18-bit, 1.5 to 2 MSPS), rather than a Sigma-Delta converter. Sigma-Delta ADCs introduce digital decimation filter group delays (often tens of microseconds) that make tight galvo position loop closure nearly impossible.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">According to research published in the <strong><a href=\"https:\/\/ieeexplore.ieee.org\/\" target=\"_blank\" rel=\"noreferrer noopener\">IEEE Transactions on Industrial Electronics<\/a><\/strong>, minimizing converter conversion latency is far more critical to galvo settling time than pushing raw oversampling resolution past 20 bits.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">The Digital PID + Feedforward Servo Loop Architecture<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">Now let&#8217;s examine the control algorithm executing inside your DSP or FPGA.<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Digital Galvo Servo Loop Structure:<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Input 1:<\/strong> Target Position Command R(k) from the trajectory generator.<\/li>\n\n\n\n<li><strong>Input 2:<\/strong> Actual Angular Feedback Y(k) from the optical sensor ADC.<\/li>\n\n\n\n<li><strong>Tracking Error Calculation:<\/strong> e(k) = R(k) &#8211; Y(k).<\/li>\n\n\n\n<li><strong>PID Processing:<\/strong> Proportional, Integral with Anti-Windup, and Band-Limited Derivative on Measurement.<\/li>\n\n\n\n<li><strong>Feedforward Addition:<\/strong> Velocity Feedforward (Kvff * V_cmd) + Acceleration Feedforward (Kaff * A_cmd).<\/li>\n\n\n\n<li><strong>Resonance Suppression:<\/strong> Cascaded 2nd-order IIR Notch Filters centered at mechanical resonance peaks.<\/li>\n\n\n\n<li><strong>Current Command Output:<\/strong> Scaled current demand sent to the DAC or PWM current-loop driver.<\/li>\n<\/ul>\n<\/blockquote>\n\n\n\n<h3 class=\"wp-block-heading\">1. Discrete PID Implementation<\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">At each sample interval Ts (e.g., 5 microseconds for a 200 kHz loop):<\/p>\n\n\n\n<ol class=\"wp-block-list\">\n<li><strong>Calculate Positional Tracking Error:<\/strong> <strong>e(k) = Target_Position(k) &#8211; Actual_Feedback(k)<\/strong><\/li>\n\n\n\n<li><strong>Proportional Term:<\/strong> <strong>P_out(k) = Kp * e(k)<\/strong><\/li>\n\n\n\n<li><strong>Integral Term with Anti-Windup:<\/strong> <strong>I_out(k) = I_out(k-1) + Ki * e(k) * Ts<\/strong><br>Clamp I_out to prevent integrator windup when large step commands saturate the coil drive amplifier.<\/li>\n\n\n\n<li><strong>Derivative Term (Filtered Derivative on Feedback):<\/strong><br>Direct derivative on error amplifies optical sensor noise. Calculate velocity feedback directly from position feedback using a low-pass filtered differentiator: <strong>D_raw(k) = Kd * ( Feedback(k) &#8211; Feedback(k-1) ) \/ Ts<\/strong><br><strong>D_filtered(k) = alpha * D_filtered(k-1) + (1 &#8211; alpha) * D_raw(k)<\/strong><\/li>\n<\/ol>\n\n\n\n<h3 class=\"wp-block-heading\">2. Adding Feedforward Control (Velocity and Acceleration)<\/h3>\n\n\n\n<p class=\"wp-block-paragraph\">A standard PID loop reacts only after an error occurs. Laser scan heads require high-speed vector tracking (e.g., vector marking at 5 m\/s without corner rounding). To eliminate following error (tracking lag), add velocity feedforward (Kvff) and acceleration feedforward (Kaff):<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Control_Output(k) = P_out(k) + I_out(k) &#8211; D_filtered(k) + ( Kvff * Velocity_Cmd(k) ) + ( Kaff * Acceleration_Cmd(k) )<\/strong><\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">Where:<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Velocity_Cmd(k)<\/strong> is the first derivative of the trajectory setpoint.<\/li>\n\n\n\n<li><strong>Acceleration_Cmd(k)<\/strong> is the second derivative of the trajectory setpoint.<\/li>\n<\/ul>\n\n\n\n<p class=\"wp-block-paragraph\">By implementing acceleration feedforward in your <strong>galvanometer scanner closed loop feedback<\/strong>, you supply the exact current needed to overcome rotor inertia before the tracking error even begins to form.<\/p>\n\n\n\n<div 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https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-2C3432-NIR-B-768x768.webp 768w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-2C3432-NIR-B-1536x1536.webp 1536w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-2C3432-NIR-B-2048x2048.webp 2048w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-2C3432-NIR-B-12x12.webp 12w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-2C3432-NIR-B-600x600.webp 600w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-2C3432-NIR-B-100x100.webp 100w\"\n\t\t\t\t\t\t\t\tsizes=\"(max-width: 2560px) 100vw, 2560px\"\n\t\t\t\t\t\t\t\tdecoding=\"async\"\n\t\t\t\t\t\t\t\talt=\"PDC-2C3432-NIR-B 2 segment fan shape segmented PIN photodiode chip\" \/>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t<\/dialog>\n\t\t<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\"><h2 class=\"wp-block-post-title\"><a href=\"https:\/\/photo-detector.com\/es\/product\/segmented-pin-photodiode-chip\/\" target=\"_blank\">Si PIN photodiodes for Galvo PDC-2C3432-NIR-B<\/a><\/h2>\n\n<div data-block-name=\"woocommerce\/product-summary\" data-is-descendent-of-single-product-block=\"true\" class=\"wp-block-woocommerce-product-summary\"><div class=\"wc-block-components-product-summary \" style=\"\">\n\t\t\t\t<p><span class=\"ng-star-inserted\">The\u00a0<\/span><strong class=\"ng-star-inserted\"><span class=\"ng-star-inserted\">PDC-2C3432-NIR-B<\/span><\/strong><span class=\"ng-star-inserted\">\u00a0is a specialized\u00a0<\/span><strong class=\"ng-star-inserted\"><span class=\"ng-star-inserted\">segmented PIN photodiode chip<\/span><\/strong><span class=\"ng-star-inserted\">\u00a0engineered for precise differential position feedback in high-speed galvanometer scanners. Integrating this dual-channel\u00a0<\/span><strong class=\"ng-star-inserted\"><span class=\"ng-star-inserted\">segmented PIN photodiode chip<\/span><\/strong><span class=\"ng-star-inserted\">\u00a0allows systems to obtain accurate angular tracking with minimal signal noise.<\/span><\/p>\n\n\t\t\t<\/div><\/div>\n\n\n<div data-block-name=\"woocommerce\/product-meta\" class=\"wp-block-woocommerce-product-meta\">\n<div class=\"wp-block-group is-nowrap is-layout-flex wp-container-core-group-is-layout-7387b849 wp-block-group-is-layout-flex\">\n\n<div class=\"taxonomy-product_tag wp-block-post-terms\"><span class=\"wp-block-post-terms__prefix\">Tag\uff1a<\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/differential-photodiode\/\" rel=\"tag\">Differential Photodiode<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/dual-segment-sensor\/\" rel=\"tag\">Dual-Segment Sensor<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/fan-shape-chip\/\" rel=\"tag\">Fan Shape Chip<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/galvo-position-detector\/\" rel=\"tag\">Galvo Position Detector<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/segmented-photodiode\/\" rel=\"tag\">Segmented Photodiode<\/a><\/div><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">Suppressing Mechanical Resonance: Digital Notch Filters<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">Every galvanometer scanner has a torsional mechanical resonance dictated by rotor inertia, mirror mount stiffness, and coil shaft compliance. This mechanical resonance typically sits between <strong>8 kHz and 22 kHz<\/strong>.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">If your loop gain pushes energy into this resonance frequency, the scan head will emit an audible squeal, overheat the drive coil, and lose position lock.<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Torsional Resonance Mechanics:<\/strong><br>At the mechanical resonance frequency f_res, the open-loop phase drops by 180 degrees while amplitude spikes by 12 dB to 25 dB. If the feedback loop attempts to correct position errors near this frequency without attenuation, the system enters self-sustaining mechanical oscillation.<\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">To stabilize your <strong>galvanometer scanner closed loop feedback<\/strong>, place one or two 2nd-order Infinite Impulse Response (IIR) Digital Notch Filters in series with your PID output:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>H_notch(z) = ( b0 + b1<em>z^-1 + b2<\/em>z^-2 ) \/ ( 1 + a1<em>z^-1 + a2<\/em>z^-2 )<\/strong><\/p>\n<\/blockquote>\n\n\n\n<p class=\"wp-block-paragraph\">Design the notch filter with:<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Center frequency (f0):<\/strong> Exactly matching the mechanical resonance measured via swept-sine frequency response analysis.<\/li>\n\n\n\n<li><strong>Quality Factor (Q):<\/strong> Between 4 and 10 to suppress the resonance peak without carving away too much phase margin around your 2 kHz to 4 kHz unity-gain crossover.<\/li>\n<\/ul>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">Driving the Coil: Current Mode Power Output Stage<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">Galvo rotors respond to <strong>torque<\/strong>, which is strictly proportional to <strong>current<\/strong> (Torque = Kt * I_coil), not voltage. Therefore, the output of your PID loop must control a high-speed transconductance (voltage-to-current) power amplifier.<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Voice Coil Transconductance Driver Stages:<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Input Command:<\/strong> Precision voltage command V_cmd from the PID loop DAC.<\/li>\n\n\n\n<li><strong>Power Operational Stage:<\/strong> High-current Class AB operational amplifier (or discrete push-pull bridge) sourcing up to 5 A to 10 A peak.<\/li>\n\n\n\n<li><strong>Current Sensing:<\/strong> Low-inductance shunt resistor (Rsense = 0.25 to 1.0 Ohm) placed in series with the galvo coil return path.<\/li>\n\n\n\n<li><strong>Inner Current Feedback:<\/strong> Inverting closed loop forcing V_sense across Rsense to strictly match V_cmd.<\/li>\n<\/ul>\n<\/blockquote>\n\n\n\n<h3 class=\"wp-block-heading\">Circuit Rules for the Power Driver:<\/h3>\n\n\n\n<ol class=\"wp-block-list\">\n<li><strong>Low Sense Resistance:<\/strong> Use a non-inductive current sense resistor (Rsense = 0.25 to 1.0 Ohm, 0.1% tolerance, 15 ppm\/\u00b0C).<\/li>\n\n\n\n<li><strong>Current Feedback Loop Speed:<\/strong> The inner current control loop should have a bandwidth at least 5 to 10 times higher than the outer position loop (typically 40 kHz to 100 kHz current loop bandwidth).<\/li>\n\n\n\n<li><strong>Thermal Dissipation:<\/strong> Galvo coils run hot during continuous vector scanning. Ensure your power amplifier stage (whether using discrete MOSFET push-pull bridges or monolithic high-voltage op-amps like the OPA548 or LM675) has a robust thermal path away from the sensitive photodiode analog front end.<\/li>\n<\/ol>\n\n\n\n<p class=\"wp-block-paragraph\">According to standard electromechanical servo design guides documented by the <strong><a href=\"https:\/\/en.wikipedia.org\/wiki\/Galvanometer\" target=\"_blank\" rel=\"noreferrer noopener\">Wikipedia Galvanometer Engineering Overview<\/a><\/strong>, closing an ultra-fast inner current loop is essential to isolate the outer <strong>galvanometer scanner closed loop feedback<\/strong> from temperature-induced coil resistance changes.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">Real-World Engineering Case: Eliminating Edge Jitter on a 20 kHz Scan Line<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">During a recent engineering review of a 3-axis galvo scan head used in wafer micromachining, the client reported intermittent 50 um ragged edges along high-speed raster scan lines.<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Failure Diagnostics Summary:<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Observed Symptom:<\/strong> Laser line edges showed periodic micro-scalloping at 100 kHz during high-acceleration raster sweeps.<\/li>\n\n\n\n<li><strong>Oscilloscope Inspection:<\/strong> A 150 mV switching spike appeared on the photodiode TIA inverting summing node, perfectly synchronized with the PWM coil drive chopping frequency.<\/li>\n\n\n\n<li><strong>Physical Root Cause:<\/strong> The TIA feedback traces for photodiode channels A and B ran across a split ground plane directly beneath the switching lines of the H-bridge coil driver. The resulting capacitive coupling injected switching ripple straight into the high-impedance inverting node of the TIA.<\/li>\n<\/ul>\n<\/blockquote>\n\n\n\n<h3 class=\"wp-block-heading\">Troubleshooting and Resolution Path:<\/h3>\n\n\n\n<ol class=\"wp-block-list\">\n<li><strong>Hardware Fix:<\/strong>\n<ul class=\"wp-block-list\">\n<li>Rerouted the photodiode signals onto an internal shielded analog layer sandwiched between solid, unbroken analog ground planes (AGND).<\/li>\n\n\n\n<li>Replaced discrete photodiode packages with the <strong><a href=\"https:\/\/photo-detector.com\/product\/segmented-pin-photodiode-chip\/\" target=\"_blank\" rel=\"noreferrer noopener\">PDC-2C3432-NIR-B dual-segment PIN photodiode chip<\/a><\/strong> to ensure both optical channels shared identical thermal and capacitive symmetry.<\/li>\n\n\n\n<li>Tuned the TIA feedback capacitor from an uncalculated 10 pF down to 1.2 pF, instantly raising front-end bandwidth from 12 kHz to 85 kHz.<\/li>\n<\/ul>\n<\/li>\n\n\n\n<li><strong>Algorithm Fix:<\/strong> Added a digital 2nd-order IIR notch filter centered at 14.2 kHz on the DSP to extinguish rotor mechanical resonance.<\/li>\n\n\n\n<li><strong>The Result:<\/strong> Positional jitter dropped from 48 microradians down to under 2.2 microradians, completely smoothing out the laser raster edges.<\/li>\n<\/ol>\n\n\n\n<p class=\"wp-block-paragraph\">This fix highlights how clean sensor physics and proper board layout are just as crucial as algorithmic tuning in any <strong>galvanometer scanner closed loop feedback<\/strong> design.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">PCB Layout and Grounding Best Practices for Galvo Servo Boards<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">When laying out your galvo servo controller board, treat the board as three distinct physical zones:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p class=\"wp-block-paragraph\"><strong>Three-Zone PCB Partitioning Scheme:<\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Zone 1 (Analog Sensor Front-End):<\/strong> Houses the Silicon PIN photodiodes, low-noise TIAs, reference voltage sources, and balanced difference amplifiers. Connected strictly to clean AGND.<\/li>\n\n\n\n<li><strong>Zone 2 (Digital Processing Core):<\/strong> Houses the 32-bit DSP \/ FPGA, high-speed SAR ADCs, digital isolators, and clock oscillators. Connected to DGND.<\/li>\n\n\n\n<li><strong>Zone 3 (Power Drive Stage):<\/strong> Houses the H-bridge \/ linear power op-amps, power supply bulk capacitors, and current sense shunts. Connected to high-current PGND.<\/li>\n<\/ul>\n<\/blockquote>\n\n\n\n<h3 class=\"wp-block-heading\">Layout Guidelines for Optimal Noise Rejection:<\/h3>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Keep TIA Inverting Traces Extremely Short:<\/strong> The trace connecting the photodiode anode\/cathode to the op-amp inverting input is the most noise-sensitive trace on the board. Make it as short as humanly possible (less than 3 mm) and surround it with an AGND guard ring.<\/li>\n\n\n\n<li><strong>Physical Thermal Isolation:<\/strong> Keep power output stages and high-power shunt resistors at the physical opposite end of the PCB from the photodiodes and TIAs. Thermal gradients across discrete photodiode pairs cause angular position drift in your <strong>galvanometer scanner closed loop feedback<\/strong>.<\/li>\n\n\n\n<li><strong>Separate AGND and PGND:<\/strong> Never return high-current coil return paths through the analog sensor ground. Tie Analog Ground (AGND), Digital Ground (DGND), and Power Ground (PGND) together only at a single star point near the power supply input.<\/li>\n\n\n\n<li><strong>Sensor Cable Shielding:<\/strong> If the optical detector head connects via a flex cable to the driver board, ensure the photodiode signal conductors are individually interleaved with ground shield traces (e.g., GND &#8211; SignalA &#8211; GND &#8211; SignalB &#8211; GND).<\/li>\n<\/ul>\n\n\n\n<div data-block-name=\"woocommerce\/single-product\" data-product-id=\"2230\" data-wp-context=\"woocommerce\/products::{&quot;productId&quot;:2230,&quot;variationId&quot;:null}\" data-wp-interactive=\"woocommerce\/single-product\" class=\"wp-block-woocommerce-single-product woocommerce\">\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-7387b849 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<div data-block-name=\"woocommerce\/product-gallery\" data-wp-context=\"{&quot;imageData&quot;:[2231],&quot;isDialogOpen&quot;:false,&quot;isDragging&quot;:false,&quot;touchStartX&quot;:0,&quot;touchCurrentX&quot;:0,&quot;productId&quot;:&quot;2230&quot;,&quot;selectedImageId&quot;:2231,&quot;thumbnailsOverflow&quot;:{&quot;top&quot;:false,&quot;bottom&quot;:false,&quot;left&quot;:false,&quot;right&quot;:false},&quot;hideNextPreviousButtons&quot;:true,&quot;isDisabledPrevious&quot;:true,&quot;isDisabledNext&quot;:true,&quot;ariaLabelPrevious&quot;:&quot;Imagen anterior&quot;,&quot;ariaLabelNext&quot;:&quot;Imagen siguiente&quot;}\" data-wp-interactive=\"woocommerce\/product-gallery\" style=\"--wc-block-product-gallery-large-image-ratio-width:1;--wc-block-product-gallery-large-image-ratio-height:1;\" class=\"wp-block-woocommerce-product-gallery wc-block-product-gallery  is-single-product-gallery-image is-layout-flex wp-container-woocommerce-product-gallery-is-layout-a2f35af1 wp-block-woocommerce-product-gallery-is-layout-flex\">\n\n\t\t\t<div data-block-name=\"woocommerce\/product-gallery-large-image\" class=\"wc-block-product-gallery-large-image wp-block-woocommerce-product-gallery-large-image\">\n\t\t\t\t\t\t\t\t\t\t\t<ul\n\t\t\t\tclass=\"wc-block-product-gallery-large-image__container\"\n\t\t\t\tdata-wp-interactive=\"woocommerce\/product-gallery\"\n\t\t\t\tdata-wp-on--keydown=\"actions.onViewerImageKeyDown\"\n\t\t\t\taria-label=\"Galer\u00eda del producto\"\n\t\t\t\ttabindex=\"0\"\n\t\t\t\taria-roledescription=\"carousel\"\n\t\t\t>\n\t\t\t\t\t\t\t\t\t<li\n\t\t\t\t\t\tclass=\"wc-block-product-gallery-large-image__wrapper\"\n\t\t\t\t\t>\n\t\t\t\t\t\t<div data-block-name=\"woocommerce\/product-image\" data-is-descendent-of-single-product-block=\"true\" data-show-product-link=\"false\" data-show-sale-badge=\"false\" class=\"wc-block-components-product-image wc-block-grid__product-image wc-block-components-product-image--aspect-ratio-auto wp-block-woocommerce-product-image\"><img fetchpriority=\"high\" decoding=\"async\" data-wp-on--click=\"actions.openDialog\" data-wp-on--mouseleave=\"actions.resetZoom\" data-wp-on--mousemove=\"actions.startZoom\" data-wp-on--touchend=\"actions.onTouchEnd\" data-wp-on--touchmove=\"actions.onTouchMove\" data-wp-on--touchstart=\"actions.onTouchStart\" data-wp-watch=\"callbacks.toggleImageVisibility\" draggable=\"false\" fetchpriority=\"high\" tabindex=\"-1\" width=\"800\" height=\"800\" src=\"https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-1024x1024.webp\" class=\"attachment-large size-large wc-block-woocommerce-product-gallery-large-image__image wc-block-woocommerce-product-gallery-large-image__image--full-screen-on-click wc-block-woocommerce-product-gallery-large-image__image--hoverZoom\" alt=\"940nm PIN Photodiode Chip for Galvo Position Feedback - Bee Photon\" data-testid=\"product-image\" data-image-id=\"2231\" style=\"object-fit:cover;\" loading=\"eager\" srcset=\"https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-1024x1024.webp 1024w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-300x300.webp 300w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-150x150.webp 150w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-768x768.webp 768w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-1536x1536.webp 1536w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-2048x2048.webp 2048w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-12x12.webp 12w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-600x600.webp 600w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-100x100.webp 100w\" sizes=\"auto, (max-width: 800px) 100vw, 800px\" \/><div class=\"wc-block-components-product-image__inner-container\"><\/div><\/div>\t\t\t\t\t<\/li>\n\t\t\t\t\t\t\t<\/ul>\n\t\t\t\t\t\t<div class=\"wc-block-product-gallery-large-image__inner-blocks\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t<\/div>\n\t\t\t\t\t<dialog inert\n\t\t\t\tdata-wp-bind--open=\"context.isDialogOpen\"\n\t\t\t\tdata-wp-bind--inert=\"!context.isDialogOpen\"\n\t\t\t\tdata-wp-on--close=\"actions.closeDialog\"\n\t\t\t\tdata-wp-on--keydown=\"actions.onDialogKeyDown\"\n\t\t\t\tdata-wp-watch=\"callbacks.dialogStateChange\"\n\t\t\t\tclass=\"wc-block-product-gallery-dialog\"\n\t\t\t\trole=\"dialog\"\n\t\t\t\taria-modal=\"true\"\n\t\t\t\taria-label=\"Product Gallery\">\n\t\t\t\t<div class=\"wc-block-product-gallery-dialog__header\">\n\t\t\t\t\t<button class=\"wc-block-product-gallery-dialog__close-button\" data-wp-on--click=\"actions.closeDialog\" aria-label=\"Cerrar ventana\">\n\t\t\t\t\t\t<svg xmlns=\"http:\/\/www.w3.org\/2000\/svg\" viewBox=\"0 0 24 24\" width=\"24\" height=\"24\" aria-hidden=\"true\" focusable=\"false\">\n\t\t\t\t\t\t\t<path d=\"M13 11.8l6.1-6.3-1-1-6.1 6.2-6.1-6.2-1 1 6.1 6.3-6.5 6.7 1 1 6.5-6.6 6.5 6.6 1-1z\"><\/path>\n\t\t\t\t\t\t<\/svg>\n\t\t\t\t\t<\/button>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"wc-block-product-gallery-dialog__content\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img\n\t\t\t\t\t\t\t\tdata-image-id=\"2231\"\n\t\t\t\t\t\t\t\tdata-wp-watch=\"callbacks.toggleImageVisibility\"\n\t\t\t\t\t\t\t\tsrc=\"https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-scaled.webp\"\n\t\t\t\t\t\t\t\tsrcset=\"https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-scaled.webp 2560w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-300x300.webp 300w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-1024x1024.webp 1024w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-150x150.webp 150w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-768x768.webp 768w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-1536x1536.webp 1536w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-2048x2048.webp 2048w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-12x12.webp 12w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-600x600.webp 600w, https:\/\/photo-detector.com\/wp-content\/uploads\/2026\/06\/PDC-C2928-NIR-B-100x100.webp 100w\"\n\t\t\t\t\t\t\t\tsizes=\"(max-width: 2560px) 100vw, 2560px\"\n\t\t\t\t\t\t\t\tdecoding=\"async\"\n\t\t\t\t\t\t\t\talt=\"940nm PIN Photodiode Chip for Galvo Position Feedback - Bee Photon\" \/>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t<\/dialog>\n\t\t<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\"><h2 class=\"wp-block-post-title\"><a href=\"https:\/\/photo-detector.com\/es\/product\/940nm-pin-photodiode-chip\/\" target=\"_blank\">Si PIN photodiodes for Galvo PDC-C2928-NIR-B<\/a><\/h2>\n\n<div data-block-name=\"woocommerce\/product-summary\" data-is-descendent-of-single-product-block=\"true\" class=\"wp-block-woocommerce-product-summary\"><div class=\"wc-block-components-product-summary \" style=\"\">\n\t\t\t\t<p>Optimize scanning with our 940nm PIN photodiode chip, PDC-C2928-NIR-B. This 940nm PIN photodiode chip ensures precise galvo position sensing and low noise.<\/p>\n\n\t\t\t<\/div><\/div>\n\n\n<div data-block-name=\"woocommerce\/product-meta\" class=\"wp-block-woocommerce-product-meta\">\n<div class=\"wp-block-group is-nowrap is-layout-flex wp-container-core-group-is-layout-7387b849 wp-block-group-is-layout-flex\">\n\n<div class=\"taxonomy-product_tag wp-block-post-terms\"><span class=\"wp-block-post-terms__prefix\">Tag\uff1a<\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/940nm-pin-photodiode\/\" rel=\"tag\">940nm PIN Photodiode<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/bee-photon\/\" rel=\"tag\">Bee Photon<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/galvo-position-sensor\/\" rel=\"tag\">Galvo Position Sensor<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/position-sensing-chip\/\" rel=\"tag\">Position Sensing Chip<\/a><span class=\"wp-block-post-terms__separator\">, <\/span><a href=\"https:\/\/photo-detector.com\/es\/product-tag\/square-silicon-photodiode\/\" rel=\"tag\">Square Silicon Photodiode<\/a><\/div><\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">Comparing Feedback Sensor Technologies<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">While optical position detectors using silicon PIN photodiodes dominate high-speed galvo scanners, understanding alternative technologies helps in choosing the right architecture for your <strong>galvanometer scanner closed loop feedback<\/strong> system.<\/p>\n\n\n\n<figure class=\"wp-block-table\"><table class=\"has-fixed-layout\"><thead><tr><th>Feature Parameter<\/th><th>Optical PIN Photodiode (BeePhoton)<\/th><th>Capacitive Position Sensor<\/th><th>Moving Magnet Inductive LVDT<\/th><\/tr><\/thead><tbody><tr><td><strong>Sensor Bandwidth<\/strong><\/td><td>Very High (&gt; 50 kHz)<\/td><td>Moderate (10 kHz to 20 kHz)<\/td><td>Low (&lt; 2 kHz)<\/td><\/tr><tr><td><strong>Angular Resolution<\/strong><\/td><td>Sub-microradian (&lt; 1 urad)<\/td><td>Sub-nanoradian (Extremely Fine)<\/td><td>Microradian<\/td><\/tr><tr><td><strong>Rotor Inertia Penalty<\/strong><\/td><td>Ultra-Low (Ultra-Lightweight Vane)<\/td><td>Low to Medium (Metal Sensor Fins)<\/td><td>High (Heavy Magnetic Core)<\/td><\/tr><tr><td><strong>Primary Drift Source<\/strong><\/td><td>Thermal \/ Emitter Aging<\/td><td>Dielectric &amp; Air Humidity Variations<\/td><td>Temperature \/ Magnetic Hysteresis<\/td><\/tr><tr><td><strong>Vibration Immunity<\/strong><\/td><td>High (Balanced Differential Die)<\/td><td>Low (Sensitive to Plate Gap Flex)<\/td><td>High<\/td><\/tr><tr><td><strong>Typical Target Application<\/strong><\/td><td>High-Speed Laser Marking &amp; OCT<\/td><td>Metrology &amp; Confocal Microscopy<\/td><td>Heavy Industrial Beam Steering<\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"wp-block-paragraph\">For applications requiring step-and-settle times under 200 microseconds, optical feedback using balanced PIN photodiode chips remains the gold standard in performance and dynamic responsiveness.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">Frequently Asked Questions (FAQ)<\/h2>\n\n\n<div id=\"rank-math-faq\" class=\"rank-math-block\">\n<div class=\"rank-math-list \">\n<div id=\"faq-question-1788249500286\" class=\"rank-math-list-item\">\n<h3 class=\"rank-math-question \">1. Why is 940 nm or 920 nm NIR preferred over visible light for galvo feedback sensors?<\/h3>\n<div class=\"rank-math-answer \">\n\n<p>Near-infrared emitters (940 nm and 920 nm) match the peak spectral responsivity of standard silicon PIN photodiodes. Furthermore, NIR LEDs generate higher optical power with lower forward voltage drops and less thermal dissipation compared to visible LEDs, keeping the scan head interior cooler and reducing photodiode thermal drift in your <strong>galvanometer scanner closed loop feedback<\/strong>.<\/p>\n\n<\/div>\n<\/div>\n<div id=\"faq-question-1788249501169\" class=\"rank-math-list-item\">\n<h3 class=\"rank-math-question \">2. How do I measure the mechanical resonance frequency of my galvo scan head?<\/h3>\n<div class=\"rank-math-answer \">\n\n<p>Send a low-amplitude swept-sine excitation signal (chirp from 100 Hz to 30 kHz) into your coil current driver while logging the position feedback signal from your ADC. Compute the Fast Fourier Transform (FFT) of the input-output transfer function. The prominent peak where feedback amplitude spikes and phase drops rapidly represents your rotor-mirror torsional resonance.<\/p>\n\n<\/div>\n<\/div>\n<div id=\"faq-question-1788249502187\" class=\"rank-math-list-item\">\n<h3 class=\"rank-math-question \">3. What causes sudden high-frequency squealing when closing the PID loop?<\/h3>\n<div class=\"rank-math-answer \">\n\n<p>This is almost always caused by one of three issues in the feedback circuitry:<br \/>1. Insufficient feedback capacitance Cf in the TIA stage, causing the front-end amplifier to oscillate.<br \/>2. Excessive proportional gain (Kp) or derivative gain (Kd) exciting the mechanical resonance peak around 10 kHz to 18 kHz.<br \/>3. Reversed feedback polarity, converting your negative feedback loop into an unstable positive feedback oscillator.<\/p>\n\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h2 class=\"wp-block-heading\">Build High-Precision Closed-Loop Optical Drivers with BeePhoton<\/h2>\n\n\n\n<p class=\"wp-block-paragraph\">Achieving sub-microradian repeatability and microsecond step response in high-speed laser scan heads demands photodetectors with rock-solid consistency, near-zero dark current, and ultra-low capacitance.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong><a href=\"https:\/\/photo-detector.com\/\" target=\"_blank\" rel=\"noreferrer noopener\">BeePhoton<\/a><\/strong> supplies high-performance silicon PIN photodiode chips and segmented quadrant arrays engineered specifically for closed-loop optical position sensing. Explore our complete range of photodiode products or speak with our sensor integration engineers to dial in the optical feedback stage for your next-generation servo driver.<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Explore Sensors:<\/strong> Browse our high-speed <strong><a href=\"https:\/\/photo-detector.com\/product\/940nm-pin-photodiode-chip\/\" target=\"_blank\" rel=\"noreferrer noopener\">940nm PIN photodiode chips<\/a><\/strong>, the ultra-fast <strong><a href=\"https:\/\/photo-detector.com\/product\/920nm-silicon-pin-photodiode\/\" target=\"_blank\" rel=\"noreferrer noopener\">920nm silicon PIN photodiodes<\/a><\/strong>, and our monolithic <strong><a href=\"https:\/\/photo-detector.com\/product\/segmented-pin-photodiode-chip\/\" target=\"_blank\" rel=\"noreferrer noopener\">segmented PIN detectors<\/a><\/strong>.<\/li>\n\n\n\n<li><strong>Get Engineering Support:<\/strong> <strong><a href=\"https:\/\/photo-detector.com\/contact-us\/\" target=\"_blank\" rel=\"noreferrer noopener\">Contact our technical team<\/a><\/strong> or email us directly at <code><strong><a href=\"mailto:info@photo-detector.com\" target=\"_blank\" rel=\"noreferrer noopener\">info@photo-detector.com<\/a><\/strong><\/code> for custom wafer dicing, optical filter matching, and <strong>galvanometer scanner closed loop feedback<\/strong> front-end consultation.<\/li>\n<\/ul>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">External References &amp; Industry Standards<\/h3>\n\n\n\n<ol class=\"wp-block-list\">\n<li>Analog Devices Technical Library: <strong><em><a href=\"https:\/\/www.analog.com\/en\/resources\/app-notes\/an-649.html\" target=\"_blank\" rel=\"noreferrer noopener\">Transimpedance Amplifier Design Handbook (AN-649)<\/a><\/em><\/strong><\/li>\n\n\n\n<li>Texas Instruments Precision Control Guides: <strong><em><a href=\"https:\/\/www.ti.com\/lit\/an\/sboa122\/sboa122.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">Compensating the Transimpedance Amplifier (SBOA122)<\/a><\/em><\/strong><\/li>\n\n\n\n<li>National Institute of Standards and Technology (NIST): <strong><em><a href=\"https:\/\/www.nist.gov\/\" target=\"_blank\" rel=\"noreferrer noopener\">Optical Sensor Calibration and Photodetector Standards<\/a><\/em><\/strong><\/li>\n\n\n\n<li>IEEE Transactions on Industrial Electronics: <strong><em><a href=\"https:\/\/ieeexplore.ieee.org\/\" target=\"_blank\" rel=\"noreferrer noopener\">Resonance Suppression and Advanced Servo Control in Galvanometer Scanners<\/a><\/em><\/strong><\/li>\n\n\n\n<li>Wikipedia: <strong><em><a href=\"https:\/\/en.wikipedia.org\/wiki\/Galvanometer\" target=\"_blank\" rel=\"noreferrer noopener\">Galvanometer Scanner Operating Principles<\/a><\/em><\/strong><\/li>\n<\/ol>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n","protected":false},"excerpt":{"rendered":"<p>If you have ever wrestled with a high-speed laser marking head drifting off-target by 200 microradians halfway through an eight-hour shift, you already know the culprit. It is almost never the digital coordinate generator or the laser source itself. The headache lives directly inside the analog-to-digital sensor chain and the servo driver circuitry. Building a [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":2381,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[1251,1249,1250,1252],"class_list":["post-2376","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-si-pin-photodiodes","tag-closed-loop-scan-head-sensor","tag-galvanometer-scanner-closed-loop-feedback","tag-galvo-servo-driver-circuit-design","tag-pid-control-loop-photodiode"],"_links":{"self":[{"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/posts\/2376","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/comments?post=2376"}],"version-history":[{"count":5,"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/posts\/2376\/revisions"}],"predecessor-version":[{"id":2382,"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/posts\/2376\/revisions\/2382"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/media\/2381"}],"wp:attachment":[{"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/media?parent=2376"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/categories?post=2376"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/photo-detector.com\/es\/wp-json\/wp\/v2\/tags?post=2376"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}