Nuclear Reaction Suite Dashboard

Interactive Nuclear Physics Calculations - Distorted Wave Born Approximation

Calculation Parameters

65 MeV
7.5 fm
0.67 fm
100 fm
Phase shifts / R-matrix / potentials integrate to this radius (if 0, API uses 100 fm). Elastic dσ uses it as R-matrix match a when > 0; 0 = automatic 2(R₀+a₀) from Woods–Saxon (same as example_alpha_Sm148_elastic.clj when that binding is commented out).

Energy ranges and channel partial waves L are on each tab: Phase Shifts, R-Matrices, and Potentials (E + L). Cross-Sections, Elastic, and Inelastic use lab energies on those tabs only (no L for σ or dσ).

Energies & partial waves
Nuclear Phase Shifts vs Energy
Energies & partial waves
R-Matrix Values Comparison
Energies & partial waves

Potentials vs r do not depend on E or L; this grid is used for the same Numerov/phase run as the other two tabs below.

Nuclear Potentials vs Radius
Energies

Total cross section uses the same E grid; the sum over L in the model uses a fixed default set (0–5) in the server — not edited here.

Total Cross-Sections vs Energy

Elastic Scattering

Computes single-channel elastic scattering for a chosen projectile + target, using the Woods–Saxon parameters above as the effective optical potential for that system. Default preset matches α + ¹⁴⁸Sm at Elab = 50 MeV (real [65, 7.5, 0.67] MeV/fm + imaginary volume WS W₀ = 30 MeV via *elastic-imag-ws-params*). Elastic dσ sums nuclear partial waves L = 0 … Lmax (default 41). Large Lmax with a strong real well plus Coulomb can inflate fN numerically (e.g. p+¹⁶O dσ/σRuth ≫ 10³); use V0=R0=0 to verify ratio ≡ 1.

Projectile kinetic in the lab; one curve per energy.

Real Woods-Saxon (V₀, R₀, a₀) from main parameters. Optional complex (optical) Woods-Saxon for absorption:

0 = real potential only
8–45; default 41 (α+¹⁴⁸Sm preset)

Ratio uses point Rutherford in the CM frame. Sanity: Coulomb-only (V0=R0=0, a0>0) ⇒ ratio 1. With the tutorial well (V0=40), raising “Max L” can explode dσ/σRuth at some angles—raise L only if you need a more converged forward nuclear term.

Elastic differential cross section

Inelastic Scattering Parameters

Like the Transfer tab, use two boxes on the left for reaction setup and on the right for entrance vs exit optical potentials. Uncheck “same exit optical” to set different distorting wells for the excited channel. Real V₀, R₀, a₀ at the entrance mirror the global sliders (below); calculation radius is shared.

Reaction & kinematics
Standard macroscopic inelastic: default channel L set in the server.
Paper mode: use beam energies as proton lab T (MeV). Requires projectile p.
Entrance channel (elastic)

Distorted wave χi and macroscopic form factor dV/dr use this Woods–Saxon.

Shared; mirrors top slider
Imaginary WS (entrance)
0 = none
Inelastic Scattering Differential Cross-Section

Transfer Reaction Parameters

Use the boxes below for transfer kinematics, separate entrance/exit bound wells (schematic zero-range), optional different imaginary parameters (echoed by the API), and radial mesh. denotes orbital multipoles in the reduced T coupling.

Kinematics & coupling
Comma-separated lab energies
Sent with energies as request L_values; multipole ℓ, not Lα
Bound state — entrance (ℓi)

Woods–Saxon for the initial overlap orbit.

Optical (imaginary) — entrance

Echoed in API; schematic path is still real kinematics only.

Radial mesh
Transfer Reaction Differential Cross-Section

Default curve (on load / when you change target or reaction type): 16O(p,d)15O at 20 MeV lab. For ¹⁶O + (d,p), the preset is ZR **¹⁶O(d,p)** (mb/sr, CM). Use Calculate for a full scan with current energies and mesh.

Energies & partial waves (same as Phase / R-matrix / Potential)
0

Data Points

0-0

Energy Range (MeV)

0

Angular Momenta

0ms

Calculation Time

Comprehensive DWBA Dashboard