21.0%-efficient co-diffused screen-printed n-type silicon solar cell with rear-side boron emitter

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Autoren

  • Nadine Wehmeier
  • Bianca Lim
  • Anja Nowack
  • Jan Schmidt
  • Thorsten Dullweber
  • Rolf Brendel

Externe Organisationen

  • Institut für Solarenergieforschung GmbH (ISFH)
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Details

OriginalspracheEnglisch
Seiten (von - bis)148-152
Seitenumfang5
Fachzeitschriftphysica status solidi (RRL) – Rapid Research Letters
Jahrgang10
Ausgabenummer2
PublikationsstatusVeröffentlicht - 22 Feb. 2016

Abstract

Plasma enhanced chemical vapor deposition (PECVD) is applied to deposit boron silicate glasses (BSG) acting as boron diffusion source during the fabrication of n-type silicon solar cells. We characterize the resulting boron-diffused emitter after boron drive-in from PECVD BSG by measuring the sheet resistances R sheet,B and saturation current densities J 0,B. For process optimization, we vary the PECVD deposition parameters such as the gas flows of the precursor gases silane and diborane and the PECVD BSG layer thickness. We find an optimum gas flow ratio of SiH 4/B 2H 6= 8% and layer thickness of 40 nm. After boron drive in from these PECVD BSG diffusion sources, a low J 0,B values of 21 fA/cm 2 is reached for R sheet,B = 70 Ω/□. The optimized PECVD BSG layers together with a co-diffusion process are implemented into the fabrication process of passivated emitter and rear totally diffused (PERT) back junction (BJ) cells on n-type silicon. An independently confirmed energy conversion efficiency of 21.0% is achieved on 15.6 × 15.6 cm 2 cell area with a simplified process flow. This is the highest efficiency reported for a co-diffused n-type PERT BJ cell using PECVD BSG as diffusion source. A loss analysis shows a small contribution of 0.13 mW/cm 2 of the boron diffusion to the recombination loss proving the high quality of this diffusion source.

ASJC Scopus Sachgebiete

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21.0%-efficient co-diffused screen-printed n-type silicon solar cell with rear-side boron emitter. / Wehmeier, Nadine; Lim, Bianca; Nowack, Anja et al.
in: physica status solidi (RRL) – Rapid Research Letters, Jahrgang 10, Nr. 2, 22.02.2016, S. 148-152.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Wehmeier N, Lim B, Nowack A, Schmidt J, Dullweber T, Brendel R. 21.0%-efficient co-diffused screen-printed n-type silicon solar cell with rear-side boron emitter. physica status solidi (RRL) – Rapid Research Letters. 2016 Feb 22;10(2):148-152. doi: 10.1002/pssr.201510393
Wehmeier, Nadine ; Lim, Bianca ; Nowack, Anja et al. / 21.0%-efficient co-diffused screen-printed n-type silicon solar cell with rear-side boron emitter. in: physica status solidi (RRL) – Rapid Research Letters. 2016 ; Jahrgang 10, Nr. 2. S. 148-152.
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title = "21.0%-efficient co-diffused screen-printed n-type silicon solar cell with rear-side boron emitter",
abstract = "Plasma enhanced chemical vapor deposition (PECVD) is applied to deposit boron silicate glasses (BSG) acting as boron diffusion source during the fabrication of n-type silicon solar cells. We characterize the resulting boron-diffused emitter after boron drive-in from PECVD BSG by measuring the sheet resistances R sheet,B and saturation current densities J 0,B. For process optimization, we vary the PECVD deposition parameters such as the gas flows of the precursor gases silane and diborane and the PECVD BSG layer thickness. We find an optimum gas flow ratio of SiH 4/B 2H 6= 8% and layer thickness of 40 nm. After boron drive in from these PECVD BSG diffusion sources, a low J 0,B values of 21 fA/cm 2 is reached for R sheet,B = 70 Ω/□. The optimized PECVD BSG layers together with a co-diffusion process are implemented into the fabrication process of passivated emitter and rear totally diffused (PERT) back junction (BJ) cells on n-type silicon. An independently confirmed energy conversion efficiency of 21.0% is achieved on 15.6 × 15.6 cm 2 cell area with a simplified process flow. This is the highest efficiency reported for a co-diffused n-type PERT BJ cell using PECVD BSG as diffusion source. A loss analysis shows a small contribution of 0.13 mW/cm 2 of the boron diffusion to the recombination loss proving the high quality of this diffusion source.",
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note = "We acknowledge Miriam Berger, Anja Christ, and Till Brendem{\"u}hl for n-PERT cell processing, Mircea Turcu for depositions and characterization of the PECVD layers, Sarah Sp{\"a}tlich for diffusion optimization and David Sylla for laser processes. This work was funded by the German Federal Ministry for Economic Affairs and Energy under Grant 0325478 (SimpliHigh).",
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Download

TY - JOUR

T1 - 21.0%-efficient co-diffused screen-printed n-type silicon solar cell with rear-side boron emitter

AU - Wehmeier, Nadine

AU - Lim, Bianca

AU - Nowack, Anja

AU - Schmidt, Jan

AU - Dullweber, Thorsten

AU - Brendel, Rolf

N1 - We acknowledge Miriam Berger, Anja Christ, and Till Brendemühl for n-PERT cell processing, Mircea Turcu for depositions and characterization of the PECVD layers, Sarah Spätlich for diffusion optimization and David Sylla for laser processes. This work was funded by the German Federal Ministry for Economic Affairs and Energy under Grant 0325478 (SimpliHigh).

PY - 2016/2/22

Y1 - 2016/2/22

N2 - Plasma enhanced chemical vapor deposition (PECVD) is applied to deposit boron silicate glasses (BSG) acting as boron diffusion source during the fabrication of n-type silicon solar cells. We characterize the resulting boron-diffused emitter after boron drive-in from PECVD BSG by measuring the sheet resistances R sheet,B and saturation current densities J 0,B. For process optimization, we vary the PECVD deposition parameters such as the gas flows of the precursor gases silane and diborane and the PECVD BSG layer thickness. We find an optimum gas flow ratio of SiH 4/B 2H 6= 8% and layer thickness of 40 nm. After boron drive in from these PECVD BSG diffusion sources, a low J 0,B values of 21 fA/cm 2 is reached for R sheet,B = 70 Ω/□. The optimized PECVD BSG layers together with a co-diffusion process are implemented into the fabrication process of passivated emitter and rear totally diffused (PERT) back junction (BJ) cells on n-type silicon. An independently confirmed energy conversion efficiency of 21.0% is achieved on 15.6 × 15.6 cm 2 cell area with a simplified process flow. This is the highest efficiency reported for a co-diffused n-type PERT BJ cell using PECVD BSG as diffusion source. A loss analysis shows a small contribution of 0.13 mW/cm 2 of the boron diffusion to the recombination loss proving the high quality of this diffusion source.

AB - Plasma enhanced chemical vapor deposition (PECVD) is applied to deposit boron silicate glasses (BSG) acting as boron diffusion source during the fabrication of n-type silicon solar cells. We characterize the resulting boron-diffused emitter after boron drive-in from PECVD BSG by measuring the sheet resistances R sheet,B and saturation current densities J 0,B. For process optimization, we vary the PECVD deposition parameters such as the gas flows of the precursor gases silane and diborane and the PECVD BSG layer thickness. We find an optimum gas flow ratio of SiH 4/B 2H 6= 8% and layer thickness of 40 nm. After boron drive in from these PECVD BSG diffusion sources, a low J 0,B values of 21 fA/cm 2 is reached for R sheet,B = 70 Ω/□. The optimized PECVD BSG layers together with a co-diffusion process are implemented into the fabrication process of passivated emitter and rear totally diffused (PERT) back junction (BJ) cells on n-type silicon. An independently confirmed energy conversion efficiency of 21.0% is achieved on 15.6 × 15.6 cm 2 cell area with a simplified process flow. This is the highest efficiency reported for a co-diffused n-type PERT BJ cell using PECVD BSG as diffusion source. A loss analysis shows a small contribution of 0.13 mW/cm 2 of the boron diffusion to the recombination loss proving the high quality of this diffusion source.

KW - Boron silicate glass

KW - Diffusion

KW - Passivated emitter and rear totally diffused solar cells

KW - Plasma enhanced chemical vapor deposition

KW - Silicon

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U2 - 10.1002/pssr.201510393

DO - 10.1002/pssr.201510393

M3 - Article

VL - 10

SP - 148

EP - 152

JO - physica status solidi (RRL) – Rapid Research Letters

JF - physica status solidi (RRL) – Rapid Research Letters

SN - 1862-6270

IS - 2

ER -

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