Layered halide perovskites

e.g. (BA)₂(MA)ₙ₋₁PbₙI₃ₙ₊₁ (BA = butylammonium, MA = methylammonium)

Also called Ruddlesden–Popper perovskites, Dion–Jacobson perovskites, (BA)₂PbI₄

van der Waals crystal semiconductor

Crystals that build their own quantum wells: sheets of lead halide separated by layers of organic molecules. They absorb and emit light strongly, and the organic spacers make them far more resistant to moisture than the 3D perovskites used in record solar cells – which is why thin 2D perovskite layers are now routinely added to perovskite solar cells to make them last longer.

Crystal structure

  • C
  • I
  • N
  • Pb
Cell
Rectangular, a = 8.88 Å, b = 8.69 Å
Atoms per cell
30
Pb–I bonds
3.18 and 3.20 Å
C–N bond
1.44 Å
C–C bonds
1.47–1.53 Å
Height
13.75 Å between the outer atom centres
One sheet of corner-sharing PbI6 octahedra, a single octahedron thick – the n = 1 member – with a layer of butylammonium cations on each face. The charged NH3+ heads sit in the pockets between octahedra, held by hydrogen bonds to iodine, and the butyl tails point outwards; tails from neighbouring layers meet across a van der Waals gap. The inorganic sheet is the quantum well and the organic layers are the barriers. Hydrogen atoms are not drawn. One layer of (C4H9NH3)2PbI4 at 293 K, from single-crystal X-ray diffraction (Billing and Lemmerer, Acta Crystallographica B 63, 735, 2007; COD 2102938): a = 8.88 Å, b = 8.69 Å. The hydrogen positions were calculated rather than measured and are left out; at room temperature the butyl chains move strongly, so their bond lengths are less precise than the lead–iodine ones.

Key properties

  • Exciton binding energies of a few hundred meV in n = 1 compounds, from combined quantum and dielectric confinement
  • Band gap tuned in steps by n, and continuously by halide and organic spacer choice
  • Much better moisture stability than 3D MAPbI3; 2D Ruddlesden–Popper solar cells retained performance for thousands of hours under illumination in 2016
  • Edges of n > 1 crystals host lower-energy states that help separate excitons into free charges
  • Soft lattice with strong electron–phonon coupling

How it is made

  • Solution processing – spin- or blade-coating of precursor inks, the route used in solar cells
  • Slow cooling or antisolvent crystallisation of millimetre-scale single crystals, followed by exfoliation
  • Treating 3D perovskite films with bulky ammonium salts to form thin 2D capping layers

Uses, and how close they are

  • Passivation and capping layers in perovskite solar cellspilot
  • Light-emitting diodes and scintillatorsprototype
  • Photodetectors and X-ray detectorsprototype

Readiness runs lab → prototype → pilot → deployed.

Open problems

  1. Can phase-pure films with a single n be deposited uniformly, instead of the mixed-n distributions typical of solution processing?
  2. How exactly do 2D layers stabilise 3D perovskite cells – chemical passivation, ion blocking or both – and do they degrade themselves?
  3. Can lead-free (for example tin-based) layered perovskites reach useful stability?

Going deeper

Short notes for specialists. Choose a lens in the header and yours comes first.

For theoreticians · your lens

Hybrid organic–inorganic structures need large cells and dynamic disorder. Spin–orbit coupling from lead is essential – it lowers the gap by roughly 1 eV – and dielectric confinement from the low-permittivity organic layers boosts exciton binding far beyond simple quantum-well estimates. Octahedral tilts and cation dynamics call for ab initio molecular dynamics; exciton–phonon coupling calls for polaron models.

For experimentalists · your lens

Determine n from low-angle XRD reflections and from the distinct excitonic absorption peak of each n – PL often reveals mixed phases that XRD misses. Control and report humidity during processing, and keep laser power densities low, since exfoliated flakes degrade under intense illumination.

For engineers · your lens

Already useful as a thin additive in perovskite photovoltaics under commercial development. As a stand-alone absorber its wide gap and poor out-of-plane transport limit efficiency; lead handling and long-term field stability remain central concerns.

In the research tracks

Recent news

The newest items tagged 2D perovskites, from the news feed updated 5 Oct 2026.

Preprintnot yet peer reviewed arXiv

Interlayer pairing mechanism for bilayer nickelate superconductors

The discovery of superconductivity in Ruddlesden-Popper bilayer nickelates under both high pressure and ambient conditions has opened a new paradigm for exploring unconventional superconductivity. This review provides a brief survey of theoretical progress on bilayer nickelate superconductors. Drawing from the key…

Preprintnot yet peer reviewed arXiv

Self-Trapping Enabled Highly Bright Momentum-Indirect Interlayer Excitons

Interlayer excitons in two dimensional material heterostructures exhibit large exciton binding energies and long lifetimes, making them ideal platforms for studying excitonic devices and many body quantum phenomena. However, the spatially separated electron and hole nature of IXs reduces their oscillator strength by…

All 6 items tagged 2D perovskites in the news feed  ·  RSS feed for 2D perovskites

Key references

  1. Atomically thin two-dimensional organic-inorganic hybrid perovskitesDou et al. · Science 349, 1518 (2015)cited by 1,380doi:10.1126/science.aac7660
  2. High-efficiency two-dimensional Ruddlesden–Popper perovskite solar cellsTsai et al. · Nature 536, 312 (2016)cited by 3,400doi:10.1038/nature18306
  3. Extremely efficient internal exciton dissociation through edge states in layered 2D perovskitesBlancon et al. · Science 355, 1288 (2017)cited by 1,109doi:10.1126/science.aal4211