Zaɓi Harshe

Gudanar da Haske Mai Ingantacciya don Kwayoyin Rana na Perovskite

Bincike kan dabarun kama haske ta amfani da yadudduka na SiO2 mai ramuka da jujjuyawar prism don inganta ingancin kwayoyin rana na perovskite sama da 20%.
solarledlight.org | PDF Size: 0.7 MB
Kima: 4.5/5
Kimarku
Kun riga kun ƙididdige wannan takarda
Murfin Takardar PDF - Gudanar da Haske Mai Ingantacciya don Kwayoyin Rana na Perovskite

Teburin Abubuwan Ciki

1. Gabatarwa

Kwayoyin rana na perovskite halide na halitta-inorganic (PSCs) sun fito a matsayin fasaha mai kawo sauyi a fannin samar da wutar lantarki daga hasken rana, inda ingancinsu ya tashi daga 3.8% zuwa kusan 20% cikin 'yan shekaru kadan. Yayin da yawancin bincike ya mayar da hankali kan inganta aikin lantarki—sufuri na masu daukar wuta, sake haduwa, da ingancin kayan—wannan takarda ta yi jayayya cewa gudanar da haske shi ne tagwayen da aka yi watsi da shi. Marubutan sun ba da shawarar wani sabon tsari ta amfani da yadudduka na SiO2 mai ramuka da jujjuyawar prism don kama haske, tare da haɗe da wani mafi kyawun oxide mai gudanar da haske (TCO) don rage sha na parasitic. Manufar: tura inganci sama da iyakokin yanzu ta hanyar daidaita fa'idodin gani da lantarki.

2. Mahimmin Fahimta: Bukatar Gudanar da Haske

Babban ra'ayin yana da sauki sosai: ba za ka iya canza abin da ba ka sha ba. A cikin PSC na yau da kullun, Layer mai aiki (CH₃NH₃PbI₃) yana sha kawai 65% na hasken da ya shiga. Sauran ana rasa su ta hanyar tunani (4%), sha na parasitic a cikin ITO (14%), da sauran yadudduka (2%). Fahimtar marubutan ita ce, ta hanyar injiniyan Layer na SiO2 na gaba tare da sifofi na ramuka da jujjuyawar prism, za su iya karkatar da haske da kama shi a cikin Layer mai aiki, suna haɓaka sha ba tare da ƙara kauri ba. Wannan dabara ce ta 'kama haske' ta gargajiya, amma an yi amfani da ita ga tsarin kayan da siraran masu sha ke da mahimmanci don tattara masu daukar wuta.

3. Tsarin Tunani: Daga Asara zuwa Kamawa

Hujjar ta bayyana a matakai uku:

  1. Gano matsalar: Asarar gani tana da yawa—14% a cikin ITO kadai. Layer mai aiki ya yi siriri da yawa don sha duk haske, duk da haka ƙara kauri yana cutar da aikin lantarki.
  2. Bayar da mafita: Yi amfani da Layer na SiO2 mai ramuka da jujjuyawar prism a gefen gilashin. Wannan tsari yana watsawa da karkatar da haske, yana ƙara tsawon hanyar gani a cikin perovskite.
  3. Tabbatar da kwaikwaiyo: Kwaikwaiyon gani (ta amfani da ma'auni daga Q. Lin et al.) ya nuna cewa tsarin da aka tsara zai iya rage tunani da sha na parasitic, yana tura sha a cikin Layer mai aiki sama da 80%.

4. Karfi da Rashi: Bincike Mai Mahimmanci

Karfi

Rashi

5. Abubuwan Da Ake Iya Aiki: Abin da Wannan ke Nufi ga Masana'antu

Ga ƙungiyoyin AR-GE, wannan takarda ita ce farkawa: injiniyan gani yana da mahimmanci kamar injiniyan kayan. Tsarin SiO2 da aka tsara za a iya haɗa su cikin layukan samar da PSC na yanzu tare da ƙaramin farashi. Ga masu saka hannun jari, ma'auni mai mahimmanci shine 'kusurwar da za a iya amfani da ita'—kewayon kusurwoyin haske da za a iya kiyaye babban inganci a kai. Idan tsarin prism mai ramuka zai iya kula da sha sama da 80% har zuwa 60°, zai zama mai canza wasa ga na'urorin hasken rana da aka haɗa cikin gini (BIPV).

6. Cikakkun Bayanai na Fasaha da Tsarin Lissafi

Ingancin kama haske yana ƙarƙashin iyakar Yablonovitch, wanda ya bayyana cewa matsakaicin abin haɓaka tsawon hanyar shine $4n^2$, inda $n$ shine ma'aunin refraction na Layer mai aiki. Ga CH₃NH₃PbI₃ ($n \approx 2.5$), iyakar ka'idar ita ce $4 \times (2.5)^2 = 25$. Tsarin prism mai ramuka da aka tsara yana kusantar wannan iyaka ta hanyar bazuwar alkiblar hasken da aka watsa.

Sha $A(\lambda)$ a cikin Layer mai aiki ana bayar da shi ta:

$$A(\lambda) = 1 - R(\lambda) - T(\lambda) - \sum_i A_i(\lambda)$$

inda $R(\lambda)$ shine tunani, $T(\lambda)$ shine watsawa, kuma $A_i(\lambda)$ shine sha na parasitic a Layer $i$. Manufar ita ce rage $R$ da $A_i$ yayin da ake haɓaka tsawon hanyar gani $L_{opt} = L_{phys} \times \text{abin haɓaka}$.

7. Sakamakon Gwaji da Bayanin Hoton Tsari

Hoto 1a yana nuna tsarin PSC na asali: gilashi / ITO (80nm) / PEDOT:PSS (15nm) / PCDTBT (5nm) / CH₃NH₃PbI₃ (350nm) / PC60BM (10nm) / Ag (100nm). Hoto 1b yana nuna sha a kan tsawon raƙuman haske ga kowane Layer. Layer mai aiki yana sha kusan 65% na bakan AM1.5G. Hoto 1c yana nuna ingancin tunani, tare da asarar 4% a fuskar gilashi-iska. Tsarin da aka tsara (ba a nuna shi a cikin ɓangaren PDF ba) zai maye gurbin gilashin lebur da Layer na SiO2 na prism mai ramuka, yana rage tunani zuwa <1% da ƙara sha na Layer mai aiki zuwa kusan 82%.

8. Tsarin Bincike: Nazarin Shari'a

Yi la'akari da PSC mai Layer mai aiki na 350nm. Ba tare da kama haske ba, sha shine 65%. Tare da tsarin prism mai ramuka, tsawon hanyar gani mai inganci ya zama $350 \text{nm} \times 4n^2 \approx 350 \times 25 = 8.75 \mu$m. Wannan yana ba da damar kusan cikakken sha na photons masu kuzari sama da tazarar band. Yawan halin yanzu na gajeren kewayawa $J_{sc}$ yana ƙaruwa daga 21 mA/cm² zuwa 26 mA/cm², yana haɓaka inganci daga 18% zuwa 22.5% (a ɗauka cewa babu canji a $V_{oc}$ ko abin cika).

9. Aikace-aikace na Gaba da Hasashen Makomai

Ka'idodin gudanar da haske a cikin wannan takarda sun wuce kwayoyin rana na perovskite. Ana iya amfani da su ga:

10. Bincike na Asali: Zurfafa Bincike

Wannan takarda tana wakiltar wani muhimmin juyi a binciken perovskite: daga inganta aikin lantarki kawai zuwa tsarin gani-lantarki gabaɗaya. Marubutan sun gano daidai cewa sha na parasitic na 14% a cikin ITO shine 'mai kashe inganci na shiru'. Duk da haka, mafitar da aka ba da shawara—SiO2 na prism mai ramuka—ba ta da ciniki. Tsarin yana ƙara matakin ƙirƙira, kuma geometry na prism na iya haifar da aikin da ya dogara da kusurwa wanda zai iya cutar da yawan makamashi na duniya. Hanya mafi ƙarfi na iya haɗa tsarin prism tare da mai nuna haske na rarraba (DBR) a gefen baya don sake amfani da photons da ba a sha ba, kamar yadda aka nuna a cikin ingantattun kwayoyin silicon (Green, 2015). Bugu da ƙari, takarda ta rasa bincike na fa'ida da farashi. Shin ribar inganci na 3-4% cikakke ya cancanci ƙarin rikitarwa? Ga kasuwanni masu daraja (misali, sararin samaniya, BIPV), eh. Ga ma'aunin amfani, watakila a'a. Filin zai amfana daga kimanta fasaha da tattalin arziki mai kama da wanda aka yi don kwayoyin PERC silicon (ITRPV, 2023).

11. Manazarta

  1. Kojima, A., Teshima, K., Shirai, Y., & Miyasaka, T. (2009). Organometal halide perovskites as visible-light sensitizers for photovoltaic cells. Journal of the American Chemical Society, 131(17), 6050-6051.
  2. Lee, M. M., Teuscher, J., Miyasaka, T., Murakami, T. N., & Snaith, H. J. (2012). Efficient hybrid solar cells based on meso-superstructured organometal halide perovskites. Science, 338(6107), 643-647.
  3. Zhou, H., Chen, Q., Li, G., Luo, S., Song, T. B., Duan, H. S., ... & Yang, Y. (2014). Interface engineering of highly efficient perovskite solar cells. Science, 345(6196), 542-546.
  4. Lin, Q., Armin, A., Nagiri, R. C. R., Burn, P. L., & Meredith, P. (2015). Electro-optics of perovskite solar cells. Nature Photonics, 9(2), 106-112.
  5. Green, M. A. (2015). Silicon solar cells: evolution, high-efficiency design and efficiency enhancements. Semiconductor Science and Technology, 30(7), 074001.
  6. ITRPV. (2023). International Technology Roadmap for Photovoltaic (ITRPV) 2022 Results. VDMA.
  7. Yablonovitch, E. (1982). Statistical ray optics. Journal of the Optical Society of America, 72(7), 899-907.