Neon (Ne)
noble-gasGas
표준 원자량
20.1797 u전자 배치
[He] 2s2 2p6녹는점
-248.59 °C끓는점
-246.05 °C밀도
0.8999 kg/m³산화 상태
0전기 음성도(Pauling)
해당 없음제1 이온화 에너지
21.564541 eV발견 연도
1898원자 반지름
160 pm상세 정보
Neon is a noble gas and the second lightest member of group 18. It is monatomic, colorless, and chemically very inert under ordinary conditions because its outer electron shell is closed. In the atmosphere it is present only as a minor constituent, but it is readily recognized by the intense reddish-orange light emitted in low-pressure electrical discharges. Its technological importance rests mainly on this optical behavior and on its cryogenic properties.
Colourless gaseous element of group 18 on the periodic table (noble gases). Neon occurs in the atmosphere, and comprises 0.0018% of the volume of the atmosphere. It has a distinct reddish glow when used in discharge tubes and neon based lamps. It forms almost no chemical compounds. Neon was discovered in 1898 by Sir William Ramsey and M.W. Travers.
The name derives from the Greek neos for "new". It was discovered from its bright orange spectral lines by the Scottish chemist William Ramsay and the English chemist Morris William Travers in 1898 from a liquefied air sample.
Neon was discovered by Sir William Ramsay, a Scottish chemist, and Morris M. Travers, an English chemist, shortly after their discovery of the element krypton in 1898. Like krypton, neon was discovered through the study of liquefied air. Although neon is the fourth most abundant element in the universe, only 0.0018% of the earth's atmosphere is neon.
From the Greek word neos, new. Discovered by Ramsay and Travers in 1898. Neon is a rare gaseous element present in the atmosphere to the extent of 1 part in 65,000 of air. It is obtained by liquefaction of air and separated from the other gases by fractional distillation.
Pure neon is a colorless, odorless, monatomic gas at ordinary temperature and pressure. When cooled below its boiling point it becomes a colorless cryogenic liquid, and at still lower temperature a solid. In a discharge tube it emits a bright red-orange glow from atomic emission lines.
Neon is best known for luminous advertising signs, indicator lamps, and decorative discharge tubes, where low-pressure neon gives a distinctive red-orange emission. Other gases or phosphors are used for many colors often called “neon” in commerce. Neon is also used in some high-voltage indicators, gas lasers such as helium-neon lasers, and specialized cryogenic applications. Liquid neon has a high refrigeration capacity per unit volume, but its cost limits broad use.
The largest use for neon gas is in advertising signs. Neon is also used to make high voltage indicators and is combined with helium to make helium-neon lasers. Liquid neon is used as a cryogenic refrigerant. Neon is highly inert and forms no known compounds, although there is some evidence that it could form a compound with fluorine.
Although neon advertising signs account for the bulk of its use, neon also functions in high-voltage indicators, lightning arrestors, wave meter tubes, and TV tubes. Neon and helium are used in making gas lasers. Liquid neon is now commercially available and is finding important application as an economical cryogenic refrigerant.
Isotopes in Earth/Planetary Science
Neon is subject to stable isotopic fractionation by physical processes, such as exchange between gas, liquid, and solid phases. Small variations in the isotope-amount ratio n(22Ne)/n(20Ne) have been used to examine gas-liquid exchange processes during groundwater recharge (water moving downward from the surface) and discharge [29] M. Ozima, F. A. Podosek. Noble Gas Geochemistry: 2nd Edition, p. 286, Cambridge University Press, Cambridge, UK (2002)., [101] Noble Gases in Geochemistry and Cosmochemistry: Reviews in Mineralogy and Geochemistry, D. Porcelli, C. J. Ballentine, and R. Wieler (Eds.), p. 844, Mineralogical Society of America and the Geochemical Society, Washington, DC (2002)., [102] F. Peeters, U. Beyerle, W. Aeschbach-Hertig, J. Holocher, M. S. Brennwald, R. Kipfer. Geochim. Cosmochim. Acta.67, 587 (2003)..
Isotopes in Geochronology
Some 21Ne and 22Ne form naturally in the Earth’s crust largely by reactions of 18O and 19F in minerals with neutrons and alpha particles emitted from uranium and thorium decay, called nucleogenic neon isotopes [29] M. Ozima, F. A. Podosek. Noble Gas Geochemistry: 2nd Edition, p. 286, Cambridge University Press, Cambridge, UK (2002)., [101] Noble Gases in Geochemistry and Cosmochemistry: Reviews in Mineralogy and Geochemistry, D. Porcelli, C. J. Ballentine, and R. Wieler (Eds.), p. 844, Mineralogical Society of America and the Geochemical Society, Washington, DC (2002).. In addition, neon isotopes can form at the surface of the Earth and in extraterrestrial bodies by cosmic-ray-induced spallation reactions on magnesium, silicon, aluminum, and sodium [103] T. E. Cerling, H. Craig. Annu. Rev. Earth Planet. Sci.22, 273 (1994)., [104] D. Lal, B. Peters. “Cosmic ray produced radioactivity on the earth”, in Cosmic Rays II, K. Sitte (Ed.), Springer-Verlag, New York (1967).. Analyses of all three stable neon isotopes may be used to distinguish these sources from primordial neon. The relative amounts of atmospheric neon and crustal nucleogenic neon isotopes in deep groundwaters and natural gases have been used in studies of solid-water-gas interactions and migration (Fig. IUPAC.10.1). The cosmogenic component is mainly detected in 21Ne and can be used to determine cosmic-ray exposure ages of rock samples, including meteorites exposed during travel through space and boulders exposed by melting of glacial ice (Fig. IUPAC.10.1).
Isotopes in Industry
Masers (Microwave Amplification by Stimulated Emission of Radiation) containing 20Ne have been used to study quantum physics. 21Ne may also play a role in maser studies of quantum physics [106] W. R. Bennett. Phys. Rev.126, 580 (1962)..
Isotopes Used as a Source of Radioactive Isotope(s)
22Ne is used to produce the radioisotope 22Na via the reaction 22Ne (p, n) 22Na [107] R. Policroniades, E. Moreno, A. Varela, G. Murillo, A. Huerta, M. E. Ortiz, E. Chávez. Rev. Mex. Fis. S.54, 46 (2008).. 20Ne has been used to produce the radioisotope 18F via the reaction 20Ne (d, 4He) 18F [107] R. Policroniades, E. Moreno, A. Varela, G. Murillo, A. Huerta, M. E. Ortiz, E. Chávez. Rev. Mex. Fis. S.54, 46 (2008)..
Neon has no stable neutral compounds known under ordinary chemical conditions. Its very high ionization energy and negligible electron affinity make conventional oxidation states chemically inaccessible. Laboratory studies have identified transient ionic or weakly bound species such as NeH⁺ and van der Waals complexes at low temperature or in plasmas, but these are not isolable bulk compounds. Neon clathrate hydrates have been reported only under suitable low-temperature, high-pressure conditions, where neon is physically trapped rather than chemically bonded.
Neon is a very inert element, however, it has been reported to form a compound with fluorine. It is still questionable if true compounds of neon exist, but evidence is mounting in favor of their existence. The ions, Ne+, (NeAr)+, (NeH)+, and (HeNe+) are known from optical and mass spectrometric studies. Neon also forms an unstable hydrate.
See more information at the Neon compound page.
Neon is not toxic and is not chemically reactive in normal use. The main hazards are physical: compressed gas cylinders can rupture if mishandled, and released gas can displace oxygen in confined spaces. Liquid neon and cold equipment can cause cryogenic burns and embrittle some materials. Discharge devices also involve electrical hazards and, in some cases, fragile glass under reduced pressure.
Atmospheric neon is chemically persistent and does not participate significantly in biological or geochemical reactions. It enters the air mainly from primordial atmospheric inventory and minor natural releases from rocks and waters; it is lost only slowly by atmospheric escape processes. Because it is inert, dilute, and nonbioaccumulative, neon has no known essential biological role and little direct ecological activity.
Commercial neon is obtained by fractional distillation of liquefied air, usually as a minor by-product of large oxygen and nitrogen production. Its low atmospheric abundance makes recovery more specialized than for argon, and purification requires separation from helium, hydrogen, and other light gases. Demand is concentrated in signage, electronics, lasers, and niche cryogenic uses. Recycling is possible from closed systems but is uncommon for small lamps and signs, so supply depends strongly on industrial gas infrastructure.
Obtained from production of liquid air as a byproduct of producing liquid oxygen and nitrogen.
Neon is a cosmically abundant light noble gas made chiefly during stellar nucleosynthesis in massive stars, especially through carbon and oxygen burning stages. It is found in the Sun, stellar atmospheres, nebulae, and planetary atmospheres, although its abundance in rocky planets is reduced by volatility and atmospheric loss. Several stable isotopes occur naturally, with ²⁰Ne dominant on Earth.
- The familiar red-orange sign color is produced by neon itself, not by a coating.
- Many commercial “neon” signs of other colors contain argon, mercury vapor, or phosphors instead.
- Neon was discovered through the fractional distillation of liquid air.
- Liquid neon is denser than liquid helium but boils at a much higher temperature.
- Neon has no known stable neutral compound at ambient conditions.
- The name comes from a Greek word meaning “new.”
이미지
특성
물리적 특성
- 원자 반지름(경험값)
- 160 pm 모든 원소의 원자 반지름(경험값) 비교 →
- 공유 결합 반지름
- 58 pm 모든 원소의 공유 결합 반지름 비교 →
- 반데르발스 반지름
- 154 pm 모든 원소의 반데르발스 반지름 비교 →
- 밀도
- 0.8999 kg/m³ 모든 원소의 밀도 비교 →
- 몰 부피
- 0.0168 L/mol
- STP에서의 상
- 기체 모든 원소의 STP에서의 상 비교 →
- 녹는점
- -248.59 °C 모든 원소의 녹는점 비교 →
- 끓는점
- -246.05 °C 모든 원소의 끓는점 비교 →
- 비열
- 1.03 J/(g·K) 모든 원소의 비열 비교 →
- 몰 열용량
- 20.786 J/(mol·K) 모든 원소의 몰 열용량 비교 →
- 결정 구조
- 면심 입방 모든 원소의 결정 구조 비교 →
화학적 특성
- 전기 음성도(Allen)
- 4.787
- 전자 친화도
- -1.2 eV (음수 값 — 추가 전자를 결합하지 않을 것으로 예측됨)
- 제1 이온화 에너지
- 21.564541 eV 모든 원소의 제1 이온화 에너지 비교 →
- 제2 이온화 에너지
- 40.963111 eV 모든 원소의 제2 이온화 에너지 비교 →
- 제3 이온화 에너지
- 63.423518 eV 모든 원소의 제3 이온화 에너지 비교 →
- 제4 이온화 에너지
- 97.190335 eV 모든 원소의 제4 이온화 에너지 비교 →
- 제5 이온화 에너지
- 126.247435 eV 모든 원소의 제5 이온화 에너지 비교 →
- 산화 상태
- 0 모든 원소의 산화 상태 비교 →
- 원자가 전자
- 8 모든 원소의 원자가 전자 비교 →
- 전자 배치
- [He] 2s2 2p6
열역학적 특성
- 삼중점(온도)
- -248.59 °C
- 삼중점(압력)
- 4.34e+4 Pa
- 임계점(온도)
- -228.658 °C
- 임계점(압력)
- 2.6786e+6 Pa
- 융해열
- 0.00347204 eV 모든 원소의 융해열 비교 →
- 기화열
- 0.01772296 eV 모든 원소의 기화열 비교 →
- 원자화열
- 0 eV
핵 특성
- 양성자 수
- 10 모든 원소의 양성자 수 비교 →
- 중성자 수
- 10 모든 원소의 중성자 수 비교 →
- 알려진 동위원소 수
- 20 모든 원소의 알려진 동위원소 수 비교 →
- 안정 동위원소 수
- 3 모든 원소의 안정 동위원소 수 비교 →
- 가장 안정한 동위원소
- Ne-20
- 발견 연도
- 1898
존재비
- 존재비(지각)
- 0.005 mg/kg 모든 원소의 존재비(지각) 비교 →
- 존재비(해양)
- 1.2 × 10−4 mg/L 모든 원소의 존재비(해양) 비교 →
결정 구조
- 격자 상수 a
- 443 pm
전자 구조
- 전자껍질별 전자 수
- 2, 8 모든 원소의 전자껍질별 전자 수 비교 →
식별자
- CAS 등록 번호
- 7440-01-9 모든 원소의 CAS 등록 번호 비교 →
- 항 기호
- 1S0
- InChI
- InChI=1S/Ne
- InChI 키
- GKAOGPIIYCISHV-UHFFFAOYSA-N
전자 배치 측정값
Ne: 2s² 2p⁶[He] 2s² 2p⁶1s² 2s² 2p⁶원자 모형
동위원소에 따라 중성자 수, 질량, 안정성은 달라지지만, 중성 원자의 전자 배치는 달라지지 않습니다.
개략적인 원자 모형이며 실제 비율과 다릅니다.
원자 지문
방출 / 흡수 스펙트럼
동위원소 분포
| 질량수 | 원자 질량(u) | 천연 존재비 | 반감기 |
|---|---|---|---|
| 20 안정 | 19.9924401762 ± 0.0000000017 | 90.4800% | 안정 |
| 21 안정 | 20.993846685 ± 0.000000041 | 0.2700% | 안정 |
| 22 안정 | 21.991385114 ± 0.000000018 | 9.2500% | 안정 |
상 / 상태
이유: 끓는점(-246.05 °C)보다 271.1 °C 높음
개략도이며 실제 비율과 다름
상전이점
전이 에너지
녹는점에서 1 mol을 녹이는 데 필요한 에너지
끓는점에서 1 mol을 기화시키는 데 필요한 에너지
밀도
표준 조건에서
현재 온도 T에서 이상 기체 법칙으로 추정
심화
원자 스펙트럼
보유 스펙트럼선 데이터 ?
| 이온 | 전하 | 총 스펙트럼선 수 | 전이 확률 | 준위 표기 |
|---|---|---|---|---|
| Ne I | 0 | 1597 | 533 | 1597 |
| Ne II | +1 | 1914 | 233 | 1912 |
| Ne III | +2 | 910 | 637 | 910 |
| Ne IV | +3 | 643 | 72 | 643 |
| Ne V | +4 | 374 | 139 | 374 |
| Ne VI | +5 | 515 | 449 | 515 |
| Ne VII | +6 | 661 | 442 | 661 |
| Ne VIII | +7 | 745 | 540 | 745 |
| Ne IX | +8 | 229 | 228 | 229 |
| Ne X | +9 | 137 | 137 | 137 |
보유 에너지 준위 데이터 ?
| 이온 | 전하 | 준위 |
|---|---|---|
| Ne I | 0 | 375 |
| Ne II | +1 | 385 |
| Ne III | +2 | 283 |
| Ne IV | +3 | 215 |
| Ne V | +4 | 161 |
| Ne VI | +5 | 135 |
| Ne VII | +6 | 208 |
| Ne VIII | +7 | 178 |
| Ne IX | +8 | 110 |
| Ne X | +9 | 149 |
화합물
동위원소 (3)
Natural neon is a mixture of three isotopes. Six other unstable isotopes are known.
| 질량수 | 원자 질량(u) | 천연 존재비 | 반감기 | 붕괴 방식 | |
|---|---|---|---|---|---|
| 20 안정 | 19.9924401762 ± 0.0000000017 | 90.4800% ± 0.0300% | 안정 | stable | |
| 21 안정 | 20.993846685 ± 0.000000041 | 0.2700% ± 0.0100% | 안정 | stable | |
| 22 안정 | 21.991385114 ± 0.000000018 | 9.2500% ± 0.0300% | 안정 | stable |
스펙트럼선
전체 1087개 중 50개를 표시합니다. 기본적으로 세기가 측정된 스펙트럼선만 표시됩니다.
| 파장(nm) | 세기 | 이온화 단계 | 유형 | 전이 | 정확도 | 출처 | |
|---|---|---|---|---|---|---|---|
| 692.94673 nm | 100000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3s 2[1/2]* → 2s2.2p5.(2P*<3/2>).3p 2[3/2] | 측정값 | NIST | |
| 703.24131 nm | 85000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<3/2>).3p 2[1/2] | 측정값 | NIST | |
| 717.39381 nm | 77000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3s 2[1/2]* → 2s2.2p5.(2P*<3/2>).3p 2[5/2] | 측정값 | NIST | |
| 724.51666 nm | 77000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<3/2>).3p 2[1/2] | 측정값 | NIST | |
| 743.88984 nm | 60000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3s 2[1/2]* → 2s2.2p5.(2P*<3/2>).3p 2[1/2] | 측정값 | NIST | |
| 702.40504 nm | 34000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3s 2[1/2]* → 2s2.2p5.(2P*<3/2>).3p 2[3/2] | 측정값 | NIST | |
| 748.88712 nm | 32000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<3/2>).3d 2[3/2]* | 측정값 | NIST | |
| 540.05618 nm | 20000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<1/2>).3p 2[1/2] | 측정값 | NIST | |
| 585.24879 nm | 20000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3s 2[1/2]* → 2s2.2p5.(2P*<1/2>).3p 2[1/2] | 측정값 | NIST | |
| 640.22472 nm | 20000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<3/2>).3p 2[5/2] | 측정값 | NIST | |
| 470.43948 nm | 15000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<3/2>).5d 2[3/2]* | 측정값 | NIST | |
| 471.20625 nm | 15000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<3/2>).6d 2[5/2]* | 측정값 | NIST | |
| 471.53441 nm | 15000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<3/2>).6d 2[7/2]* | 측정값 | NIST | |
| 650.65281 nm | 15000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<3/2>).3p 2[5/2] | 측정값 | NIST | |
| 470.88584 nm | 12000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<3/2>).5d 2[1/2]* | 측정값 | NIST | |
| 453.77551 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<1/2>).5d 2[3/2]* | 측정값 | NIST | |
| 471.00638 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<3/2>).5d 2[1/2]* | 측정값 | NIST | |
| 478.89249 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<3/2>).7s 2[3/2]* | 측정값 | NIST | |
| 482.73382 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<3/2>).6s 2[3/2]* | 측정값 | NIST | |
| 488.49181 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<1/2>).5d 2[5/2]* | 측정값 | NIST | |
| 495.70324 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[3/2] → 2s2.2p5.(2P*<1/2>).5d 2[5/2]* | 측정값 | NIST | |
| 534.10932 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<3/2>).4d 2[1/2]* | 측정값 | NIST | |
| 588.18952 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<1/2>).3p 2[1/2] | 측정값 | NIST | |
| 602.99969 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<1/2>).3p 2[1/2] | 측정값 | NIST | |
| 607.43377 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<3/2>).3p 2[1/2] | 측정값 | NIST | |
| 614.30626 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<3/2>).3p 2[3/2] | 측정값 | NIST | |
| 616.35939 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3s 2[1/2]* → 2s2.2p5.(2P*<1/2>).3p 2[1/2] | 측정값 | NIST | |
| 621.72812 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<3/2>).3p 2[3/2] | 측정값 | NIST | |
| 626.6495 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3s 2[1/2]* → 2s2.2p5.(2P*<1/2>).3p 2[3/2] | 측정값 | NIST | |
| 633.44278 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<3/2>).3p 2[5/2] | 측정값 | NIST | |
| 638.29917 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<3/2>).3p 2[3/2] | 측정값 | NIST | |
| 659.89529 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3s 2[1/2]* → 2s2.2p5.(2P*<1/2>).3p 2[1/2] | 측정값 | NIST | |
| 705.91074 nm | 10000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<1/2>).3d 2[3/2]* | 측정값 | NIST | |
| 576.44189 nm | 7000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<3/2>).4d 2[7/2]* | 측정값 | NIST | |
| 533.07771 nm | 6000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<3/2>).4d 2[3/2]* | 측정값 | NIST | |
| 534.3282 nm | 6000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<3/2>).4d 2[1/2]* | 측정값 | NIST | |
| 597.5534 nm | 6000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3s 2[3/2]* → 2s2.2p5.(2P*<1/2>).3p 2[3/2] | 측정값 | NIST | |
| 475.27311 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<3/2>).6d 2[7/2]* | 측정값 | NIST | |
| 479.02171 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3p 2[3/2] → 2s2.2p5.(2P*<1/2>).6d 2[5/2]* | 측정값 | NIST | |
| 483.73128 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[1/2] → 2s2.2p5.(2P*<3/2>).6s 2[3/2]* | 측정값 | NIST | |
| 489.20896 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[3/2] → 2s2.2p5.(2P*<3/2>).7s 2[3/2]* | 측정값 | NIST | |
| 500.51582 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[3/2] → 2s2.2p5.(2P*<1/2>).5d 2[5/2]* | 측정값 | NIST | |
| 503.77504 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<3/2>).5d 2[7/2]* | 측정값 | NIST | |
| 514.49371 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3p 2[3/2] → 2s2.2p5.(2P*<1/2>).5d 2[5/2]* | 측정값 | NIST | |
| 514.50308 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<1/2>).3p 2[3/2] → 2s2.2p5.(2P*<1/2>).5d 2[5/2]* | 측정값 | NIST | |
| 556.27668 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<1/2>).4d 2[5/2]* | 측정값 | NIST | |
| 565.66578 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[3/2] → 2s2.2p5.(2P*<1/2>).4d 2[5/2]* | 측정값 | NIST | |
| 571.92256 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[3/2] → 2s2.2p5.(2P*<1/2>).4d 2[5/2]* | 측정값 | NIST | |
| 574.82979 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<3/2>).4d 2[5/2]* | 측정값 | NIST | |
| 580.44496 nm | 5000 | Ne I | emission | 2s2.2p5.(2P*<3/2>).3p 2[5/2] → 2s2.2p5.(2P*<3/2>).4d 2[5/2]* | 측정값 | NIST |
확장 특성
공유 결합 반지름(확장)
- 공유 결합 반지름(Pyykkö)
- 67 pm
- 공유 결합 반지름(Pyykkö, 이중 결합)
- 96 pm
반데르발스 반지름
- Bondi
- 154 pm
- Alvarez
- 158 pm
- UFF
- 324.3 pm
- MM3
- 160 pm
원자 및 금속 반지름
- 원자 반지름(Rahm)
- 156 pm
번호 척도
- Mendeleev
- 113
- Pettifor
- 2
- Glawe
- 2
전기 음성도 척도
- Ghosh
- 0
- Gunnarsson–Lundqvist
- 7
- Robles–Bartolotti
- 7
분극률 및 분산
- 쌍극자 분극률
- 2.6611 a.u.
- 쌍극자 분극률(불확도)
- 0 a.u.
- C₆
- 6.2 Ha·Bohr6
- C₆ (Gould–Bučko)
- 6.91 Ha·Bohr6
화학 친화력
- 양성자 친화도
- 198.8 kJ/mol
- 기체상 염기성
- 174.4 kJ/mol
비활성 기체 특성
상전이 및 동소체
| 녹는점 | 24.56 K |
| 끓는점 | 27.1 K |
| 임계점(온도) | 44.49 K |
| 임계점(압력) | 2.68 MPa |
| 삼중점(온도) | 24.56 K |
| 삼중점(압력) | 43.37 kPa |
심화 참고 데이터
차폐 상수 (3)
| n | 오비탈 | σ |
|---|---|---|
| 1 | s | 0.3579 |
| 2 | p | 4.2416 |
| 2 | s | 4.2416 |
동위원소 붕괴 방식 (35)
| 동위원소 | 모드 | 세기 |
|---|---|---|
| 15 | 2p | 100% |
| 16 | 2p | 100% |
| 17 | B+ | 100% |
| 17 | B+p | 94.4% |
| 17 | B+A | 3.5% |
| 17 | B+pA | 0% |
| 18 | B+ | 100% |
| 19 | B+ | 100% |
| 23 | B- | 100% |
| 24 | B- | 100% |
X선 산란 인자 (503)
| 에너지 (eV) | f₁ | f₂ |
|---|---|---|
| 10 | — | 0 |
| 10.1617 | — | 0 |
| 10.3261 | — | 0 |
| 10.4931 | — | 0 |
| 10.6628 | — | 0 |
| 10.8353 | — | 0 |
| 11.0106 | — | 0 |
| 11.1886 | — | 0 |
| 11.3696 | — | 0 |
| 11.5535 | — | 0 |
추가 데이터
Estimated Crustal Abundance
The estimated element abundance in the earth's crust.
5×10-3 milligrams per kilogram
참고 문헌 (1)
Estimated Oceanic Abundance
The estimated element abundance in the earth's oceans.
1.2×10-4 milligrams per liter
참고 문헌 (1)
참고 문헌
(9)
Data deposited in or computed by PubChem
The half-life and atomic mass data was provided by the Atomic Mass Data Center at the International Atomic Energy Agency.
Element data are cited from the Atomic weights of the elements (an IUPAC Technical Report). The IUPAC periodic table of elements can be found at https://iupac.org/what-we-do/periodic-table-of-elements/. Additional information can be found within IUPAC publication doi:10.1515/pac-2015-0703 Copyright © 2020 International Union of Pure and Applied Chemistry.
The information are cited from Pure Appl. Chem. 2018; 90(12): 1833-2092, https://doi.org/10.1515/pac-2015-0703.
Thomas Jefferson National Accelerator Facility (Jefferson Lab) is one of 17 national laboratories funded by the U.S. Department of Energy. The lab's primary mission is to conduct basic research of the atom's nucleus using the lab's unique particle accelerator, known as the Continuous Electron Beam Accelerator Facility (CEBAF). For more information visit https://www.jlab.org/
The periodic table at the LANL (Los Alamos National Laboratory) contains basic element information together with the history, source, properties, use, handling and more. The provenance data may be found from the link under the source name.
The periodic table contains NIST's critically-evaluated data on atomic properties of the elements. The provenance data that include data for atomic spectroscopy, X-ray and gamma ray, radiation dosimetry, nuclear physics, and condensed matter physics may be found from the link under the source name. Ref: https://www.nist.gov/pml/atomic-spectra-database
This section provides all form of data related to element Neon.
The element property data was retrieved from publications.