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First-magnitude star

A first-magnitude star is one of the brightest stars observable to the naked eye from Earth, defined as having an apparent visual magnitude of 1.50 or brighter (i.e., a numerical value of 1.50 or less). There are currently 22 such stars in the night sky, a count that remains stable due to the fixed nature of stellar positions and brightnesses over human timescales. The brightest of these is Sirius in the constellation Canis Major, shining at an apparent magnitude of -1.46. The classification system for these stars traces its origins to the ancient Greek astronomer , who around 150 BCE developed the earliest known magnitude scale by grouping visible stars into six classes based on their perceived , with first-magnitude denoting the most prominent ones. 's qualitative approach, later refined by in the , assigned the brightest 20 or so stars to the first magnitude without precise measurements, relying instead on visual estimation. In the 19th century, British astronomer Norman Pogson formalized the scale in 1856, introducing a logarithmic basis where a difference of one magnitude corresponds to a brightness ratio of approximately 2.512, and a five-magnitude difference equates to a factor of 100 in ; this allowed first-magnitude stars to be precisely defined relative to a standard, such as at magnitude 0.03. These stars hold significant cultural and practical importance, serving as key navigational aids for centuries—such as (magnitude 1.97, just outside first magnitude but often associated) for northern latitude determination—and forming the basis of many constellations in ancient astronomy. Notable examples include (-0.74, the second-brightest and a beacon), (-0.05, the brightest in the northern sky), (0.03, a zero-magnitude standard), and (0.18, a in ). Their apparent brightness results from a combination of intrinsic , , and interstellar extinction, with distances ranging from nearby Alpha Centauri (4.37 light-years) to distant ones like (over 2,600 light-years). Observations from missions like have refined their magnitudes to high precision, confirming the list and aiding studies of and galactic structure.

Historical Origins

Hipparchus's Star Catalog

, an active around 190–120 BCE, is credited with compiling the first known systematic , which included approximately 850 stars with their positions and brightness classifications. This , now lost, represented a groundbreaking effort in , conducted primarily from where worked. His work laid the empirical foundation for later celestial mapping by providing a structured inventory of , enabling comparisons over time and influencing generations of astronomers. The motivation for Hipparchus's catalog stemmed from his observation of a , or "new star," in 134 BCE, an unprecedented event that challenged the prevailing view of the heavens as unchanging. Struck by this phenomenon, which appeared suddenly and then faded, Hipparchus initiated systematic observations to document stellar positions and brightnesses, aiming to detect future anomalies. This , likely visible from , prompted what is considered the earliest comprehensive stellar survey, emphasizing the importance of baseline data in astronomy. In his catalog, Hipparchus pioneered the division of stars into six classes based on apparent brightness, with first-magnitude stars designated as the brightest visible to the naked eye and sixth-magnitude stars as the faintest detectable without aid. This qualitative scale relied on visual estimation, grouping stars by relative luminosity rather than precise measurement, and marked the origin of the magnitude system still in use today. The modern apparent magnitude scale refines this approach logarithmically for quantitative precision. Hipparchus's catalog profoundly influenced subsequent astronomers, particularly Claudius in the 2nd century CE, who incorporated and adapted much of it into his own work. preserved Hipparchus's stellar data in the , expanding the catalog to about 1,025 entries while retaining the six-magnitude brightness scheme, thus ensuring the survival and dissemination of Hipparchus's innovations through the medieval period. This transmission solidified the magnitude classification as a cornerstone of astronomical tradition.

Ancient to Modern Magnitude Evolution

The magnitude classification for began with Hipparchus's division of visible into six brightness classes in the BCE, serving as the foundational for later refinements. In the CE, Claudius Ptolemy refined this approach in his , a comprehensive astronomical that cataloged over ,000 while preserving the six- scale from brightest (first ) to faintest visible (sixth ). Ptolemy's assessments relied on subjective visual judgments of apparent , without quantitative ratios between classes, leading to inconsistencies when compared to standards; for instance, his magnitudes often deviated by up to from photoelectric values due to personal perception and atmospheric effects. This emphasized qualitative ranking for naked-eye observers, influencing astronomical practice for centuries despite its limitations in precision. Medieval Islamic astronomers built upon Ptolemy's work, with Abd al-Rahman al-Sufi in the 10th century expanding star catalogs in his while retaining the Hipparchian six-magnitude scale. Observing from around 964 , al-Sufi incorporated finer subdivisions, such as one-third magnitude steps (e.g., denoting stars as "between 5 and 6"), and updated magnitudes for about 45% of entries through independent observations, correcting for and with an estimated of 0.057 magnitudes per airmass. His catalog of roughly 1,028 stars enhanced the system's applicability across Islamic scholarly traditions, bridging with later European revivals by providing more detailed brightness estimates than Ptolemy's originals. The marked a shift toward greater observational rigor, exemplified by Brahe's 16th-century naked-eye measurements at his observatory. Brahe compiled a catalog of 1,004 stars by 1598, assigning integer magnitudes from 1 to 6 with occasional qualifiers for finer gradations, achieving positional accuracies of about 2 arcminutes— an better than predecessors— through instruments like the mural quadrant. His magnitudes correlated closely with modern values, with errors typically under 0.5 magnitudes, demonstrating the potential of systematic visual photometry without optical aids and laying groundwork for Kepler's later analyses. The brought scientific standardization when British astronomer Norman Pogson proposed a in , calibrating the ancient system to quantitative terms where a difference of 5 magnitudes corresponds to a 100:1 in (). This definition aligned with the perceived logarithmic response of the , establishing each magnitude step as a factor of approximately 2.512 in intensity, formalized by the equation: m_1 - m_2 = -2.5 \log_{10} \left( \frac{b_2}{b_1} \right) where m_1 and m_2 are the magnitudes, and b_1 and b_2 are the corresponding brightnesses. Pogson's scale was rapidly adopted, transforming subjective rankings into a precise tool for comparing stellar luminosities. The 20th century transitioned to objective methods with the advent of photoelectric photometry, pioneered by Joel Stebbins at the University of Illinois Observatory from 1907 to 1922. By replacing selenium cells with more sensitive photoelectric tubes around 1914, Stebbins enabled accurate flux measurements of variable stars like Algol, achieving precisions far surpassing visual estimates (down to 0.01 magnitudes). This technique became the standard for determining stellar magnitudes, quantifying light in absolute terms and eliminating observer bias, thus revolutionizing photometry into a cornerstone of modern astrophysics.

Magnitude System Fundamentals

Apparent Magnitude Scale

The apparent magnitude, denoted as m, quantifies the brightness of a celestial object as observed from Earth, reflecting the flux received by an observer without regard to the object's distance. This measure is essential for comparing the observed luminosities of stars and other astronomical bodies in the night sky. The apparent magnitude scale is logarithmic, a design that compresses the vast range of stellar brightnesses into a manageable numerical system. Each interval of one magnitude corresponds to a brightness ratio of approximately 2.512, derived from Pogson's ratio, which is the fifth root of 100 (\sqrt{{grok:render&&&type=render_inline_citation&&&citation_id=5&&&citation_type=wikipedia}}{100} \approx 2.512). This standardization ensures that a decrease in magnitude by 5 units represents a 100-fold increase in brightness. The zero point is calibrated using the star Vega, which has an apparent magnitude of 0.03 in the visual band (V magnitude), serving as the reference for the scale across optical wavelengths. Brighter objects receive negative magnitudes, as exemplified by Sirius at -1.46, while fainter ones have positive values that increase with diminishing brightness. The relationship between magnitudes and fluxes is expressed by the formula: \Delta m = -2.5 \log_{10} \left( \frac{f_1}{f_2} \right) where \Delta m is the magnitude difference and f_1, f_2 are the fluxes of two objects. This equation underpins the scale's logarithmic nature, allowing astronomers to compute brightness ratios precisely from magnitude measurements. Unlike apparent magnitude, which depends on both a star's intrinsic luminosity and its distance from Earth, absolute magnitude (M) assesses intrinsic brightness by standardizing the distance to 10 parsecs, enabling direct comparisons of stellar luminosities.

Naked-Eye Visibility Thresholds

Under ideal dark-sky conditions, the human can detect stars down to an of approximately 6.5 to 7.0, allowing observers to see thousands of stars on clear nights. This limit represents the threshold of visual sensitivity for point sources like stars against a dark background, with exceptional observers potentially reaching magnitude 7.6 or fainter in pristine environments. First-magnitude stars, defined as those with an of 1.50 or brighter, form the uppermost tier of naked-eye luminosity and stand out prominently even under compromised viewing conditions. These stars, including examples like Sirius and , remain easily discernible in areas with moderate , where fainter objects fade from view. On the Bortle dark-sky scale, first-magnitude stars are visible in class 6 skies (bright suburban sky), where the naked-eye is approximately 5.5, and even in class 7 skies (suburban/urban transition) with a limiting magnitude of about 5.0, ensuring their reliability for casual observation. Several factors modulate the visibility of these stars beyond sky quality alone. Atmospheric extinction, caused by and in Earth's atmosphere, progressively dims stars as they approach the horizon, with effects most pronounced at low altitudes. Light pollution from artificial sources elevates sky brightness, reducing contrast for all but the brightest objects. Additionally, individual observer characteristics, such as age-related decline in and overall eye health, can raise the personal by 1 or more units compared to younger, healthier individuals. The enduring visibility of first-magnitude stars has cemented their cultural importance across civilizations. They served as key navigational aids, with guiding mariners in the and southern bright stars like aiding equatorial and southern voyages. In mythology, these prominent lights inspired stories and constellations, symbolizing deities, heroes, and seasonal cycles in traditions from to Indigenous Australian .

Catalog of First-Magnitude Stars

Definition and Selection Criteria

A first-magnitude star is defined as one with an apparent visual magnitude (V) of 1.50 or brighter, corresponding to m_V ≤ 1.50 on the modern logarithmic scale of stellar brightness. This criterion establishes the brightest category of naked-eye visible stars, distinguishing them from fainter second-magnitude stars (1.50 < m_V ≤ 2.50). The apparent magnitude measures the star's brightness as observed from Earth, incorporating both its intrinsic luminosity and distance. The concept traces back to the ancient Greek astronomer around 129 BCE, who classified the approximately 20 brightest stars in his catalog as "of the first ," a qualitative ranking that roughly aligns with modern values of m_V < 1.5 for those objects. In contemporary astronomy, this historical grouping has been refined and quantified through photoelectric photometry, a technique that uses electronic detectors to measure light intensity precisely through standard filters, ensuring consistent V-band values across observations. This method replaced earlier visual estimates, providing the accuracy needed for the current definition. Selection criteria strictly apply to stars alone, excluding non-stellar objects such as , , or deep-sky entities like galaxies and nebulae. Variable stars are included based on their mean over a cycle, rather than instantaneous values, to reflect typical visibility. As of 2025, high-precision astrometric data from the satellite and mission confirm 22 such stars meeting these standards. Edge cases highlight the precision of the 1.50 cutoff: (α Eridani), with m_V = 0.46, is unequivocally first-magnitude due to its exceptional brightness, while Elnath (β Tauri), at m_V = 1.65, falls into the second-magnitude category despite its prominence in . These examples underscore how modern measurements resolve ambiguities in borderline brightness levels.

List of the 22 Brightest Stars

The 22 first-magnitude stars, defined as those with apparent visual magnitudes of 1.50 or brighter, represent the most prominent points of light in the visible to the under dark conditions. These stars span a range of spectral types from hot blue giants to cool red supergiants and are located at distances from just over 4 light-years to more than 2,000 light-years. The list below is ordered by increasing and draws from astronomical catalogs including and DR3 for positions, magnitudes, and distances, with no significant revisions to this ranking since the 2022 Gaia data release.
Common NameBayer DesignationConstellationApparent Magnitude (V)Spectral TypeDistance (ly)Notes
Siriusα CMaCanis Major-1.46A1V8.6Main-sequence star; binary with white dwarf companion (Sirius B)
Canopusα CarCarina-0.74F0II310Yellow-white supergiant; emits X-rays from hot corona
Alpha Centauriα CenCentaurus-0.27G2V + K1V4.4Triple system; closest star system to the Sun, includes Proxima Centauri
Arcturusα BooBoötes-0.05K0III37Red giant; high proper motion relative to the Sun
Vegaα LyrLyra0.03A0V25Blue-white main-sequence star; surrounded by dusty debris disk
Capellaα AurAuriga0.08G3III + G5III43Binary system of yellow giants; spectroscopic binary
Rigelβ OriOrion0.18B8Ia860Blue supergiant; multiple star system with companions
Procyonα CMiCanis Minor0.38F5IV-V11.5Subgiant; binary with white dwarf companion (Procyon B)
Achernarα EriEridanus0.46B3Vpe140Rapidly rotating Be star; oblate spheroid shape due to rotation
Betelgeuseα OriOrion0.50 (var.)M2Iab548Red supergiant; semi-regular variable; potential supernova candidate; binary system with a faint A-type companion discovered in 2025
Hadarβ CenCentaurus0.61 (var.)B1III393Blue giant; close eclipsing binary system
Altairα AqlAquila0.77A7V17Main-sequence star; rapid rotation causes oblate shape
Acruxα CruCrux0.77B0.5IV + B1V321Binary system of blue subgiants; visual double
Aldebaranα TauTaurus0.86 (var.)K5III65Orange giant; lies in foreground of Hyades open cluster
Antaresα ScoScorpius0.96 (var.)M1.5Iab550Red supergiant; binary with hot B-type companion
Spicaα VirVirgo0.98 (var.)B1V + B2V250Close spectroscopic binary of blue main-sequence stars
Polluxβ GemGemini1.14K0III34Orange giant; one of the nearest giants to Earth
Fomalhautα PsAPiscis Austrinus1.16A3V25Main-sequence star; debris disk with imaged exoplanet candidate
Becruxβ CruCrux1.25 (var.)B0.5III280Blue giant; Beta Cephei-type pulsating variable
Denebα CygCygnus1.25A2Ia2,600White supergiant; one of the most luminous stars known
Regulusα LeoLeo1.35B7V79Blue-white main-sequence star; quadruple system
Adharaε CMaCanis Major1.50B2II431Blue giant; binary system with hot companion
These stars exhibit diverse astrophysical characteristics that highlight stages. For instance, Sirius and are nearby main-sequence stars with companions, remnants of evolved solar-like stars that have exhausted their core hydrogen. In contrast, distant supergiants like and are massive, evolved stars with luminosities thousands of times that of , their brightness sustained despite great distances. Variable stars among them, such as and , show semi-regular pulsations due to internal instabilities in their extended envelopes.

Sky Distribution Patterns

Celestial Coordinates and Coverage

The equatorial coordinates of first-magnitude stars, expressed in right ascension (RA) and (Dec) for the epoch J2000.0, provide a framework for locating these prominent objects on the . measures eastward along the from the , in hours, minutes, and seconds, while measures north or south of the , in degrees, arcminutes, and arcseconds. These coordinates reveal the stars' fixed positions relative to axis, enabling precise mapping despite the annual of the equinoxes. Observations from missions like and have refined these to high precision as of 2024. The following table lists the 22 traditional first-magnitude stars (apparent magnitude ≤1.5), ordered by brightness, with their approximate RA and Dec derived from the Hipparcos and Gaia catalogues. This selection encompasses all stars visible to the unaided eye under dark skies, spanning a magnitude range from -1.46 to 1.50.
RankStar NameConstellationApparent MagnitudeRA (h m s)Dec (° ' ")
1SiriusCanis Major-1.4606 45 09-16° 42′ 58″
2CanopusCarina-0.7206 23 57-52° 41′ 44″
3Rigil KentaurusCentaurus-0.29 (combined)14 39 36-60° 50′ 02″
4ArcturusBoötis-0.0514 15 39+19° 10′ 57″
5VegaLyrae0.0318 36 56+38° 47′ 01″
6CapellaAurigae0.0805 16 41+45° 59′ 53″
7RigelOrionis0.1305 14 32-08° 12′ 06″
8ProcyonCanis Minoris0.3407 39 18+05° 13′ 30″
9AchernarEridani0.4601 37 43-57° 14′ 12″
10BetelgeuseOrionis0.50 (variable)05 55 10+07° 24′ 25″
11HadarCentauri0.61 (combined)14 03 49-60° 22′ 23″
12AltairAquilae0.7719 50 47+08° 52′ 06″
13AcruxCrucis0.77 (combined)12 26 36-63° 05′ 57″
14AldebaranTauri0.8604 35 55+16° 30′ 33″
15AntaresScorpii0.96 (variable)16 29 24-26° 25′ 55″
16SpicaVirginis0.9813 25 12-11° 09′ 41″
17PolluxGeminorum1.1407 45 19+28° 01′ 34″
18FomalhautPiscis Austrini1.1622 57 39-29° 37′ 20″
19DenebCygni1.25 (variable)20 41 26+45° 16′ 49″
20MimosaCrucis1.2512 47 43-59° 41′ 20″
21RegulusLeonis1.3510 08 22+11° 58′ 02″
22AdharaCanis Majoris1.5006 58 38-28° 58′ 19″
These coordinates demonstrate an uneven distribution across the , with a notable concentration of first-magnitude stars near the of the . This clustering arises from the higher density of stars within the galactic disk, where interstellar dust and gas also enhance the visibility of brighter, closer objects; naked-eye stars are thus more abundant along the Milky Way's band than in polar regions. Several first-magnitude stars lie in proximity to the , the plane of projected onto the sky, which coincides with the zodiac belt used in ancient astronomy. Examples include in , in , in , and in , whose positions near this path allowed early observers to track planetary motions against a backdrop of fixed bright points. In terms of coverage, the 22 stars span all four celestial quadrants but show a bias toward the southern sky, with 12 having negative declinations south of the —such as at -52.7°, at -63.1°, and Hadar at -60.4°—reflecting the Milky Way's orientation and the greater number of observable bright stars from southern latitudes. Conceptual visualizations of these positions highlight recognizable patterns, such as the asterism formed by Sirius (RA 06h 45m, Dec -16.7°), (RA 07h 39m, Dec +5.2°), and (RA 05h 55m, Dec +7.4°), which creates an prominent in the northern winter sky and underscores the geometric clustering of these beacons.

Hemispheric Visibility Differences

Observers in the , such as at a of 40°N, can view 16 of the 22 first-magnitude stars at some point during the year, but several prominent southern stars remain below the horizon. These include Canopus (δ ≈ -52°), (δ ≈ -57°), Alpha Centauri (δ ≈ -60°), Hadar (δ ≈ -60°), (δ ≈ -63°), and (δ ≈ -59°), which are inaccessible due to their southerly declinations exceeding the visible limit of approximately -50° from that latitude. In contrast, observers in the at 40°S enjoy access to all 22 first-magnitude stars over the course of the seasons, as the northernmost of these stars, such as (δ ≈ +46°), lies within the visible sky's upper limit of about +50°. This affords unique perspectives on southern constellations, including the stars and , which form part of the iconic Southern Cross and are never visible from northern latitudes above about 30°N. Among first-magnitude stars, none are truly from mid-northern latitudes like 40°N, where such stars would require declinations greater than +50°; however, the nearby second-magnitude (δ ≈ +89°) serves as a classic northern example. In the at 40°S, several first-magnitude stars qualify as , including , , Alpha Centauri, Hadar, , and (all with δ < -50°), while the southern , , is much fainter at magnitude 5.5. Seasonal variations further influence hemispheric views, with stars rising and setting according to . For instance, from the , Sirius reaches its highest point in the winter sky, appearing prominently overhead during evening hours in and . In modern astronomy, factors like light travel times from these stars (ranging from 4 to over 2,600 light-years) and have negligible impacts on current visibility patterns, as proper motions are small and shifts occur over millennia, with changes imperceptible within a human lifetime.

First-Magnitude Deep-Sky Objects

First-magnitude deep-sky objects refer to non-stellar entities, including galaxies, nebulae, and star clusters, that exhibit an integrated of 1.5 or brighter, making them among the most luminous extended features visible in the . Unlike the point-like appearance of individual , these objects present as diffuse patches or hazy glows due to their vast sizes and distributed light sources, often spanning degrees across the sky. This extended nature distinguishes them from the 21 first-magnitude , which are resolved as discrete points even to the . Historically, such objects were sometimes cataloged ambiguously in early astronomical records, with diffuse galaxies or nebulae mistaken for unresolved star groups or atmospheric phenomena before telescopic observations clarified their compositions. The (LMC) stands as the preeminent example of a first-magnitude , a barred irregular with an integrated of 0.1, spanning approximately 10 degrees in angular size and located about 163,000 light-years away in the constellations and . As a of the , the LMC's brightness arises from its roughly 10 billion stars, interspersed with nebulae and clusters, creating a luminous, mottled patch visible to the under . Its proximity and scale make it a key target for studying galactic interactions, though its full extent requires wide-field views to appreciate. Another notable instance is the (NGC 3372), an immense complex with an integrated magnitude of 1.0, extending over 120 arcminutes in the southern constellation Carina and situated about 8,500 light-years distant. This star-forming region, energized by massive young stars including the , glows prominently due to ionized hydrogen emissions, appearing as a bright, irregular cloud that rivals the in scale but surpasses it in total luminosity. While galaxies and nebulae like these are rare at first-magnitude levels—primarily confined to southern skies—several open star clusters also achieve this threshold through their collective stellar output. For instance, the Hyades cluster in integrates to magnitude 0.5 across its V-shaped , comprising over 200 stars at a distance of about 153 light-years, though its loose structure blends seamlessly with foreground stars like . Similarly, the Alpha Persei Cluster (Collinder 39) reaches magnitude 1.2, forming a 6-degree-wide group around the star Mirfak, visible as a subtle enhancement in the constellation's stellar field. These clusters highlight how deep-sky brightness can mimic stellar patterns, leading to early cataloging challenges where boundaries between resolved stars and unresolved groups were unclear. Observation of first-magnitude deep-sky objects is optimized from latitudes south of 20° N, where the LMC and rise high overhead during austral summer, revealing their intricate details even without optical aid on moonless nights with low . or wide-field telescopes enhance resolution of their extended features, such as the LMC's bar and spiral arms or the 's dark lanes, underscoring their value in demonstrating the system's application to composite celestial structures beyond isolated stars.

Variable Stars Among First-Magnitude

Among the 21 first-magnitude stars, four are known to be , meaning their apparent magnitudes fluctuate over time due to intrinsic physical processes within the stars themselves. These include (α Orionis), which varies between 0.0 and 1.6 magnitudes as a semiregular ; (α Tauri), a slow irregular varying by about 0.2 magnitudes from 0.75 to 0.95; (α Scorpii), an irregular with a range of 0.6 to 1.6 magnitudes; and (α Virginis), a short-period with a small variation of 0.97 to 1.04 magnitudes. The primary types of variability among these stars are pulsating and eclipsing binary. Pulsating variables, such as Betelgeuse, Aldebaran, and Antares, undergo periodic expansions and contractions of their outer layers, leading to changes in luminosity and temperature. The larger red giants and supergiants like Betelgeuse and Antares exhibit semiregular or irregular pulsations with longer timescales—Betelgeuse has a dominant period of around 400 days, though its behavior is not strictly periodic—resulting from complex interactions in their convective envelopes. Spica's variability arises from its close binary nature, causing minor eclipses. These variability mechanisms have significant full amplitude ranges and periods that distinguish them from non-variable first-magnitude stars. For pulsating types, the instability strip mechanism triggers kappa- and gamma-driven pulsations, where opacity changes from ionized metals and helium cause the stellar radius to vary by up to 10-20% in extreme cases like Betelgeuse, producing amplitude swings of over 1 magnitude. None of these stars exhibit large rotational modulation or eclipsing variability at first-magnitude levels beyond the listed types; for example, Algol (β Persei) is an eclipsing binary but ranges from 2.1 to 3.4 magnitudes, placing it outside the first-magnitude category. Ongoing monitoring by organizations like the American Association of Variable Star Observers (AAVSO) and the European Space Agency's mission provides precise photometric data for these stars, enabling detailed analysis. AAVSO's network has amassed thousands of observations for alone, tracking its irregular cycles, while 's high-precision and photometry (from Data Release 3 and beyond) reveal microvariations with uncertainties below 0.01 magnitudes. As of 2025, no first-magnitude star has permanently varied beyond the +1.50 magnitude threshold defining the group, though transient dimmings—such as 's 2019-2020 event to near 1.5—have occurred without long-term expulsion. The presence of these variables challenges historical astronomical assumptions of fixed stellar magnitudes, as codified in early catalogs like Ptolemy's , where brightness was treated as constant. This variability complicates naked-eye navigation and historical records but enhances our understanding of , particularly for evolved giants nearing the end of their lives. For instance, Betelgeuse's pulsations offer insights into mass loss and potential precursors, underscoring the dynamic nature of even the brightest night-sky beacons.

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