{"id":8490,"date":"2026-04-24T19:55:27","date_gmt":"2026-04-24T11:55:27","guid":{"rendered":"https:\/\/www.ledtestsystem.com\/?p=8490"},"modified":"2026-04-24T19:55:27","modified_gmt":"2026-04-24T11:55:27","slug":"precision-wavelength-analysis-tools","status":"publish","type":"post","link":"https:\/\/ledtestsystem.com\/ko\/%eb%b8%94%eb%a1%9c%ea%b7%b8-2\/precision-wavelength-analysis-tools\/","title":{"rendered":"Precision Wavelength Analysis Tools"},"content":{"rendered":"<h2>Foundational Principles of Wavelength Accuracy in Radiometric Systems<\/h2>\n<p>The measurement of optical radiation across the ultraviolet, visible, and infrared spectra demands instruments capable of resolving wavelength positions with sub-nanometer precision. Precision wavelength analysis tools serve as the cornerstone for evaluating spectral power distributions (SPDs), chromaticity coordinates, color rendering indices (CRI\/ R1\u2013R15), and correlated color temperature (CCT) in a wide array of photonic technologies. In the context of modern solid-state lighting, the shift toward narrowband emitters\u2014such as phosphor-converted white LEDs, quantum dot displays, and laser-driven phosphors\u2014has amplified the necessity for spectroradiometers that maintain calibration stability across temporal and thermal variations. A fundamental requirement for any precision wavelength analysis system is the ability to correct for spectral stray light, detector nonlinearity, and wavelength shift due to ambient temperature fluctuations. These corrections are not optional; they are mandatory for compliance with international standards such as CIE 13.3, CIE 015:2018, IES LM-79-19, and SAE J2657 for automotive lighting. The <a href=\"https:\/\/www.lisungroup.com\/\" target=\"_blank\" rel=\"noopener\">\ub9ac\uc21c<\/a> LPCE-2 (LISUN LPCE-2 <a href=\"https:\/\/www.lisungroup.com\/products\/led-test-instruments\/high-precision-spectroradiometer-integrating-sphere-system.html\" target=\"_blank\" rel=\"noopener\">\uc801\ubd84\uad6c<\/a> and Spectroradiometer System) exemplifies a hardware\u2013software architecture engineered to address these exacting requirements, employing a double-monochromator design with a photodiode array (PDA) detector that simultaneously captures 2048 spectral channels from 380 nm to 780 nm, with wavelength accuracy rated at \u00b10.3 nm.<\/p>\n<h2>Spectroradiometric Architecture: The LPCE-2 and LPCE-3 System Design<\/h2>\n<p>Both the LISUN LPCE-2 and LPCE-3 integrate a high-reflectivity barium sulfate (BaSO\u2084) coated <a href=\"https:\/\/www.lisungroup.com\/products\/led-test-instruments\/high-precision-spectroradiometer-integrating-sphere-system.html\" target=\"_blank\" rel=\"noopener\">\uc801\ubd84 \uad6c<\/a> with a calibrated spectroradiometer, but the distinguishing factor lies in the detector configuration and dynamic range. The LPCE-2 utilizes a back-thinned CCD array with a 16-bit A\/D converter, providing a spectral resolution of 0.2 nm per pixel and a signal-to-noise ratio (SNR) exceeding 1000:1 at the reference wavelength. The LPCE-3, in contrast, incorporates a cooled InGaAs photodiode array for near-infrared (NIR) extension up to 1100 nm, which is essential for photovoltaic quantum efficiency measurements and OLED emission characterization where phosphorescence peaks frequently appear beyond the visible range. Both systems incorporate a built-in shutter mechanism for dark current subtraction, and the optical fiber coupling geometry is designed to minimize self-absorption effects within the sphere\u2014a critical consideration when testing high-power LEDs (\u226510 W) that generate significant thermal load. The sphere diameters are configurable from 0.3 m to 2.0 m, allowing compliance with the 4\u03c0 measurement conditions stipulated in LM-79 for total luminous flux measurements. The wavelength calibration is maintained via an internal mercury-argon (Hg-Ar) spectral line source that performs automatic recalibration at user-defined intervals, correcting for any drift caused by thermal expansion of the grating or detector aging. This closed-loop calibration protocol ensures that the wavelength axis remains traceable to NIST and PTB standards over extended operational periods.<\/p>\n<h2>High-Precision Testing Protocols for LED and OLED Manufacturing<\/h2>\n<p>In LED wafer fabrication and die-level characterization, the ability to resolve spectral emission from individual chips is paramount for binning according to the ANSI C78.377 standard for chromaticity chromaticity quadrants. The LPCE-2\u2019s CCD array captures a complete SPD in a single integration cycle, which is crucial for pulsed-mode testing where the electrical driving current is modulated at frequencies up to 500 kHz to evaluate transient thermal effects on phosphor conversion. The system\u2019s high-speed mode achieves acquisition rates of 20 spectra per second, enabling statistical analysis of flicker and color shift during ramp-up and steady-state operation. For OLED panel testing, where the emission layers often exhibit microcavity effects causing angle-dependent spectral shifts, the spectroradiometer must be paired with a goniophotometer accessory. The LPCE-2 software suite includes a virtual goniometer module that mathematically deconvolves the far-field intensity distribution from near-field measurements, allowing manufacturers to compute average color uniformity across a 120\u00b0 viewing angle without mechanical movement of the panel. The system\u2019s stray light correction algorithm, based on a 32\u00d732 matrix deconvolution kernel, reduces measurement error in the deep-blue region (400\u2013440 nm) to less than 0.5%, which is particularly relevant for UV-LED curing systems used in additive manufacturing and medical photopolymerization.<\/p>\n<h2>Automotive Lighting Compliance and Dual-Beam Headlamp Characterization<\/h2>\n<p>The automotive lighting sector has experienced a paradigm shift with the adoption of adaptive driving beam (ADB) systems and matrix LED headlamps that require precise photometric and colorimetric evaluation at multiple test points as specified in UN Regulation R149 and SAE J3069. The LPCE-2 and LPCE-3 are deployed in test laboratories for measuring the chromaticity of low-beam and high-beam patterns, where the CCT must remain within 3500 K to 6000 K to avoid glare-induced driver fatigue. The integrating sphere\u2019s baffle design minimizes direct illumination of the sphere wall by the primary optical beam, while the spectroradiometer\u2019s stray light suppression of 10\u207b\u2075 at 10 nm away from the principal emission line ensures accurate measurement of the yellow-blue ratio (Y\/B) used to assess color fog-threshold. For automotive interior accent lighting\u2014where individual RGB LEDs are pulse-width modulated to create ambient color transitions\u2014the LPCE-2\u2019s time-resolved spectroscopy mode (100 \u00b5s temporal resolution) captures the instantaneous SPD during PWM cycles, calculating the effective CRI and CCT as a function of duty cycle. The system can automatically generate the automotive-grade test reports required for ECE R112 and R123 certification, including polar plots of color overangle within the \u00b130\u00b0 horizontal viewing zone mandated for tail lamps and turn signals.<\/p>\n<h2>Aerospace and Aviation Lighting: High-Altitude and Low-Temperature Performance Validation<\/h2>\n<p>Aviation lighting applications, ranging from runway edge lights to anti-collision beacons on aircraft wings, demand spectroradiometric accuracy under extreme environmental conditions. The LPCE-3, with its extended NIR capability, is particularly suited for evaluating tungsten-halogen and LED-based navigation lights that must comply with Federal Aviation Administration (FAA) Advisory Circular 150\/5345-53D and International Civil Aviation Organization (ICAO) Annex 14 standards. These standards mandate that the chromaticity coordinates of obstruction lights must remain within the aviation red (R, G, B) boundaries even at ambient temperatures as low as \u221240\u00b0C. The LPCE-3\u2019s cooling system maintains the detector at \u221210\u00b0C, reducing dark current noise to &lt;0.01 counts per second, which is critical when measuring the weak spectral tails of filtered red LEDs at temperatures where the forward voltage and emission peak shift by up to 2 nm. Furthermore, the system\u2019s fiber-optic input allows the spectrometer module to be placed outside the environmental chamber while the integrating sphere is exposed to thermal cycling, eliminating temperature-induced drift in the detector electronics. Data from these tests directly inform the design of aviation-grade LED luminaires that must maintain consistent color identification from distances exceeding 10 nautical miles.<\/p>\n<h2>Display Equipment Metrology: MicroLED and MiniLED Color Uniformity<\/h2>\n<p>The advent of MicroLED and MiniLED display technologies has introduced stringent requirements for per-pixel wavelength accuracy, as pixel-to-pixel variation in emission wavelength of even 1 nm results in perceptible mura artifacts. The LPCE-2 offers a microspectrometry mode where a fiber bundle with a 50 \u00b5m core diameter is coupled to the integrating sphere, allowing the capture of SPDs from submillimeter emitting areas. The system\u2019s mathematical deconvolution of the instrument\u2019s slit function\u2014modeled as a Voigt profile with a full-width at half-maximum (FWHM) of 1.5 nm\u2014enables extraction of the true spectral linewidths of quantum dot emission layers, which typically have an FWHM of 20\u201330 nm. For OLED television panels, where the white point is synthesized via blue pump layers and yellow phosphors, the LPCE-2 software automatically calculates the \u0394uv color deviation from the D65 standard, using the CIE 1976 UCS diagram for small-color-difference evaluation. The system also supports the VESA DisplayHDR True Black standard, validating that the black-level CCT remains below 0.01 cd\/m\u00b2 without color shift to blue\u2014an effect caused by residual leakage current in thin-film transistors. The combined temporal and spectral resolution allows engineers to correlate pixel aging with spectral degradation over 1000-hour accelerated life tests.<\/p>\n<h2>Photovoltaic Industry Application: Spectral Mismatch Correction for Solar Simulators<\/h2>\n<p>In the photovoltaic (PV) sector, accurate measurement of spectral irradiance is essential for calculating the spectral mismatch correction factor (MMF) when calibrating reference cells against primary standards per IEC 60904-3 and ASTM E927-19. The LPCE-3\u2019s NIR extension to 1100 nm covers the entire absorption range of crystalline silicon (c-Si) cells, while its UV sensitivity down to 300 nm supports thin-film technologies such as cadmium telluride (CdTe) and copper indium gallium selenide (CIGS). The integrating sphere serves as a spectral irradiance monitor inside the solar simulator test plane, capturing the SPD from 300 nm to 1100 nm in less than 100 ms. The system\u2019s software automatically computes the MMF using the measured SPD and the reference cell\u2019s quantum efficiency (QE) data, reducing calibration uncertainty from \u00b12% to \u00b10.5%. For concentrator photovoltaic (CPV) systems that require spectral matching under highly non-uniform illumination, the LPCE-3\u2019s cosine-corrected diffuser accessory ensures angular acceptance of \u00b185\u00b0, meeting the requirements of IEC 62670-3. The wavelength calibration traceability is verified quarterly using the LPCE-3\u2019s internal Hg-Ar source, which emits 13 identifiable spectral lines across the detection range, with the 546.1 nm mercury line used as the primary reference.<\/p>\n<h2>Scientific Research and Optical Instrument R&amp;D: Variable Resolution Spectroscopy<\/h2>\n<p>Research laboratories developing new phosphor materials, laser phosphors, or perovskite quantum dots require spectroradiometers that offer flexibility in integration time and spectral resolution. The LPCE-2 provides user-selectable electronic gain from 1\u00d7 to 64\u00d7, allowing signal optimization for very low luminance levels (down to 0.001 cd\/m\u00b2) encountered in bioluminescence and fluorescence decay measurements. The operating software includes a peak detection algorithm that locates emission maxima with sub-pixel interpolation, achieving centroid accuracy better than 0.05 nm for isolated spectral lines. This capability is instrumental in the characterization of rare-earth-doped phosphors such as YAG:Ce\u00b3\u207a, where the emission centroid shifts are correlated with crystal field splitting. For instrumentation developers designing their own optical measurement systems, the LPCE-2\u2019s raw data export format (ASCII and CSV) includes detector pixel mapping and calibrated wavelength axis, enabling custom post-processing in MATLAB or Python. The stray light correction matrix can be disabled for research purposes, allowing scientists to study the intrinsic behavior of optical components without algorithmic modification.<\/p>\n<h2>Urban Lighting Design and Mesopic Vision Parameters<\/h2>\n<p>Urban lighting designers increasingly specify LED streetlights based on mesopic luminous efficacy parameters as defined in CIE 191:2010, which accounts for the eye\u2019s spectral sensitivity under intermediate adaptation levels (0.005 to 5.0 cd\/m\u00b2). The LPCE-2 spectroradiometer provides direct measurement of scotopic\/photopic (S\/P) ratio by integrating the SPD weighted by the V'(\u03bb) and V(\u03bb) functions. Modern urban fixtures employing phosphor-converted white LEDs typically exhibit S\/P ratios between 1.8 and 2.5, significantly higher than high-pressure sodium (HPS) lamps (S\/P \u2248 0.6). The system\u2019s dynamic range of 10\u2076 enables accurate measurement of both the peak luminance of the fixture and the background sky glow spectral contributions simultaneously. For smart city lighting controls that dim fixtures to 10% output during off-peak hours, the LPCE-2\u2019s low-light sensitivity ensures that CIE chromaticity coordinates remain reliable even at 0.1% of full output. Compliance with EN 13201-5 requires that the SPD be measured under actual dimming conditions, and the LPCE-2 software automatically generates the required photometric data sheets including CCT, CRI, and TM-30 metrics (Rf, Rg, Rcs).<\/p>\n<h2>Marine and Navigation Lighting: Salt Fog and Vibration Robustness<\/h2>\n<p>Navigation lights for maritime applications (COLREGS Annex I) must maintain their chromaticity within specified boundaries even after prolonged exposure to saline atmospheres and vibration from marine engines. The LPCE-3 system, constructed with an IP65-rated fiber-optic connector and hermetically sealed detector housing, is suitable for integration into environmental test chambers where the sphere is subjected to salt fog per ASTM B117 while the spectroradiometer remains in a controlled environment. For LED-based marine lanterns that use Fresnel lenses to achieve 360\u00b0 horizontal beam patterns, the system measures the spatial distribution of CCT by rotating the fixture on a goniometer while capturing an SPD at every 5\u00b0 increment. The resulting data are processed to generate iso-CCT contour maps, which are essential for verifying that the lantern\u2019s color does not become yellow or green due to chromatic aberration in the lens material. The LPCE-2\u2019s internal reference detector monitors any drift in the sphere\u2019s reflectance during long-term tests exceeding 1000 hours, automatically compensating for any degradation.<\/p>\n<h2>Stage and Studio Lighting: High-CRI and Tunable White Systems<\/h2>\n<p>Entertainment lighting applications in stage, film, and broadcast environments demand spectroradiometers that can validate the color fidelity of tunable white and RGBAW fixtures under varying dimming curves. The LPCE-2\u2019s high-speed mode is particularly valuable for capturing the SPD of xenon strobes and LED pixel walls where pulse durations are as short as 50 \u00b5s. The software includes a CIE 13.3-2012 color rendering index module that evaluates R9 (saturated red) and R13 (skin tone), which are often compromised in commercial LED fixtures optimized for lumen output rather than color quality. For studio lighting where multiple fixtures are ganged to produce a composite white point, the system can overlay up to 10 SPDs on the same graph and compute the resultant chromaticity using additive color mixing theory. The LPCE-2\u2019s ability to output the TM-30-20 color vector graphic (CVG) provides designers with a visual representation of hue shifts in the 16 hue bins, enabling rapid adjustment of individual LED string currents to achieve a target spectral composition.<\/p>\n<h2>Medical Lighting Equipment: Surgical and Dental Curing Light Validation<\/h2>\n<p>Medical lighting\u2014including surgical overhead lamps, dental curing lights, and phototherapy devices\u2014requires rigorous spectral validation per IEC 60601-2-41 (general medical lighting) and ISO 10650 (dental curing units). The LPCE-2\u2019s absolute irradiance calibration, traceable to NIST, allows direct measurement of irradiance (W\/m\u00b2) at the target plane, which is critical for ensuring that blue-light curing units operating at 450\u2013490 nm deliver the necessary dosage without causing retinal phototoxicity. For surgical shadowless lamps that must maintain a CCT of 4000\u20135000 K, the system measures color temperature over the entire illuminated field using a 2D mapping accessory. The wavelength stability envelope\u2014less than 0.3 nm over a 24-hour warm-up period\u2014ensures that photodynamic therapy (PDT) lasers tuned to 630 nm or 690 nm can be certified for clinical use. The software includes a spectral irradiance limit analysis according to ANSI Z136.1 for laser hazards, automatically flagging any deviation beyond the maximum permissible exposure (MPE) thresholds.<\/p>\n<h2>Comparative Analysis of LPCE-2 and LPCE-3 Performance Specifications<\/h2>\n<p>The following table summarizes the key parameters distinguishing the two platforms:<\/p>\n<table>\n<thead>\n<tr>\n<th>\ub9e4\uac1c\ubcc0\uc218<\/th>\n<th>LPCE-2<\/th>\n<th>LPCE-3<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td>Spectral Range<\/td>\n<td>380\u2013780 nm<\/td>\n<td>300\u20131100 nm<\/td>\n<\/tr>\n<tr>\n<td>\ud0d0\uc9c0\uae30<\/td>\n<td>Back-thinned CCD (2048 pixels)<\/td>\n<td>Cooled InGaAs PDA (512 pixels) + CCD<\/td>\n<\/tr>\n<tr>\n<td>\ud30c\uc7a5 \uc815\ud655\ub3c4<\/td>\n<td>\u00b10.3 nm (Hg-Ar calibrated)<\/td>\n<td>\u00b10.5 nm (NIR: \u00b11.0 nm)<\/td>\n<\/tr>\n<tr>\n<td>FWHM Resolution<\/td>\n<td>1.5 nm<\/td>\n<td>2.0 nm (visible), 5.0 nm (NIR)<\/td>\n<\/tr>\n<tr>\n<td>\ub2e4\uc774\ub098\ubbf9 \ub808\uc778\uc9c0<\/td>\n<td>10\u00b3 (16-bit ADC)<\/td>\n<td>10\u2074 (18-bit ADC)<\/td>\n<\/tr>\n<tr>\n<td>SNR at 550 nm<\/td>\n<td>1000:1<\/td>\n<td>800:1 (visible), 500:1 (NIR)<\/td>\n<\/tr>\n<tr>\n<td>Sphere Diameters Available<\/td>\n<td>0.3 m, 0.5 m, 1.0 m, 1.5 m, 2.0 m<\/td>\n<td>0.3 m, 0.5 m, 1.0 m, 2.0 m<\/td>\n<\/tr>\n<tr>\n<td>Typical Application<\/td>\n<td>LED\/OLED, display, automotive visible<\/td>\n<td>PV, NIR OLED, thermal emitter<\/td>\n<\/tr>\n<tr>\n<td>Stray Light Correction<\/td>\n<td>32\u00d732 matrix deconvolution<\/td>\n<td>64\u00d764 matrix deconvolution<\/td>\n<\/tr>\n<tr>\n<td>\uc778\ud130\ud398\uc774\uc2a4<\/td>\n<td>USB 3.0, Ethernet<\/td>\n<td>USB 3.0, Ethernet, RS-232<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>The LPCE-3\u2019s extended NIR capability makes it the preferred choice for photovoltaic testing and OLED degradation studies where emission shifts into the 800\u20131000 nm region, while the LPCE-2\u2019s higher optical resolution in the visible band is optimal for color-critical applications in display and automotive lighting.<\/p>\n<h2>Standards Compliance and Calibration Traceability Infrastructure<\/h2>\n<p>Both the LPCE-2 and LPCE-3 are supplied with a calibration certificate traceable to the National Institute of Standards and Technology (NIST) via a spectrally flat deuterium-halogen transfer standard. The calibration process involves four independent stages: (1) wavelength calibration using an internal Hg-Ar lamp with 13 discrete lines; (2) absolute irradiance calibration via a 1000 W FEL-type quartz halogen lamp calibrated for spectral irradiance from 250 nm to 2500 nm; (3) spectral response linearity verification using a double-aperture method yielding &lt;1% linearity error over 10\u2075 dynamic range; and (4) stray light correction matrix generation using a 470 nm notch filter. For customers requiring ISO\/IEC 17025 accreditation, the system outputs a measurement uncertainty budget including contributions from sphere coating degradation (0.5% per year), detector quantum efficiency drift (0.2% per year), and wavelength shift (0.1 nm per year). The recommended recalibration interval is 12 months, with an optional in-field calibration check using the internal light source at 6-month intervals.<\/p>\n<h2>Frequently Asked Questions<\/h2>\n<p><strong>Q1: What is the practical difference between the LPCE-2 and LPCE-3 for LED streetlight testing?<\/strong><br \/>\nThe LPCE-2 provides higher wavelength resolution (1.5 nm FWHM) in the visible range, which is crucial for accurately determining the S\/P ratio and TM-30 color fidelity metrics that urban lighting designers require. The LPCE-3 extends into the NIR, but for typical phosphor-converted white LEDs, the LPCE-2\u2019s dynamic range and SNR in the 380\u2013780 nm band are sufficient for mesopic photometry.<\/p>\n<p><strong>Q2: Can the LPCE-2 measure absolute spectral radiance (W\/sr\/m\u00b2) in addition to flux?<\/strong><br \/>\nYes. When configured with the optional luminance adapter (a cosine-corrected input optic), the measuring software directly computes spectral radiance in units of W\u00b7sr\u207b\u00b9\u00b7m\u207b\u00b2\u00b7nm\u207b\u00b9. The sphere must be replaced with a flat reflectance standard for radiance measurements; the software automatically scales the calibration factor based on the sphere diameter or aperture.<\/p>\n<p><strong>Q3: How does the system handle pulsed or modulated light from automotive LED lamps?<\/strong><br \/>\nThe LPCE-2 offers a time-resolved mode with 100 \u00b5s minimum integration time, enabling capture of individual PWM cycles. The software triggers on the rising edge of the electrical drive signal (using the BNC trigger input) and accumulates spectra aligned to the modulation phase. For high-frequency modulation exceeding 2 kHz, the system can average over 128 cycles to reconstruct the equivalent continuous SPD.<\/p>\n<p><strong>Q4: What environmental conditions are specified for the integrating sphere coating?<\/strong><br \/>\nThe BaSO\u2084 coating maintains &gt;97% diffuse reflectance from 400 nm to 1500 nm, with a temperature coefficient of \u22120.001% per degree Celsius. The coating is hygroscopic; long-term storage below 60% relative humidity is recommended. The sphere mounts include a desiccant cartridge that is user-replaceable. For extreme humidity environments (marine, tropical), the LPCE-3\u2019s optional PTFE-lined sphere offers &lt;0.5% humidity absorption.<\/p>\n<p><strong>Q5: Is the LPCE-2 compatible with the IES LM-79-19 darkroom goniophotometer method?<\/strong><br \/>\nYes. The LPCE-2 can be integrated as the measurement head in a Type C goniophotometer. The software supports both the absolute photometry and relative photometry modes described in LM-79-19, automatically computing the spatial distribution of CCT, CRI, and Duv in addition to total flux. The system outputs the IES:LM-63 standard file format for photometric data exchange.<\/p>","protected":false},"excerpt":{"rendered":"<p>Foundational Principles of Wavelength Accuracy in Radiometric Systems The measurement of optical radiation across the ultraviolet, visible, and infrared spectra demands instruments capable of resolving wavelength positions with sub-nanometer precision. Precision wavelength analysis tools serve as the cornerstone for evaluating spectral power distributions (SPDs), chromaticity coordinates, color rendering indices (CRI\/ R1\u2013R15), and correlated color temperature [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":3432,"comment_status":"closed","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[1113],"class_list":["post-8490","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-blogs","tag-instrument-for-measuring-wavelength"],"_links":{"self":[{"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/posts\/8490","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/comments?post=8490"}],"version-history":[{"count":1,"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/posts\/8490\/revisions"}],"predecessor-version":[{"id":8491,"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/posts\/8490\/revisions\/8491"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/media\/3432"}],"wp:attachment":[{"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/media?parent=8490"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/categories?post=8490"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/ledtestsystem.com\/ko\/wp-json\/wp\/v2\/tags?post=8490"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}