Phosphorous doping in the nc-Si network
induces gradually reduced
crystallinity; however, preferential growth along <220>-oriented
crystallites promotes the columnar-like growth morphology. At optimum
doping, substitution by donor P+-atoms in the c-Si lattice
contributes surplus free electrons and high carrier mobility, resulting
in superior electrical conductivity in the n-nc-Si
network. An elevated doping leads to incorporating elemental P0 atoms in the interstitial position or forming P–Si–H
clusters and generating voids between the crystalline columns. Segregation
of defects contributes to decreasing carrier mobility and reducing
conductivity after diminishing crystallinity and narrowing the optical
band gap. By precisely controlling the growth at 250 °C and efficient
electrically active doping by P+-atoms, n-nc-Si thin films with superior dark conductivity (∼101 S cm–1) are produced in which the percolation
of charge carriers through the crystalline columns could facilitate
stacked-layer devices. The optimum n-nc-Si thin films
are used as the emitter layers in n-nc-Si/p-c-Si heterojunction solar cells (HJSCs). Furthermore,
an ultrathin a-Si:H buffer layer on the p-c-Si minimizes
the junction carrier recombination loss, and subsequent postdeposition
short-time H-plasma treatment (PSHPT) ensures seeds for superior nanocrystallization
in the n-nc-Si emitter layer. The n-nc-Si/(PSHPT)i-nc-Si(buffer layer)/p-c-Si HJSC delivers a PV conversion efficiency, η ∼12.35%,
via a reasonable fill factor of ∼0.647 and sensible JSC of ∼32.75 mA cm–2. Further improvement
in the PV performance could be possible using suitably thinner p-c-Si wafers, harmonizing with the effective carrier diffusion
length, and fabricating a high-quality passivation structure on the
backside.