diff --git a/Examples/Tests/CMakeLists.txt b/Examples/Tests/CMakeLists.txt
index c4713123ae6..7d67666bb0b 100644
--- a/Examples/Tests/CMakeLists.txt
+++ b/Examples/Tests/CMakeLists.txt
@@ -70,6 +70,7 @@ add_subdirectory(resampling)
 add_subdirectory(restart)
 add_subdirectory(restart_eb)
 add_subdirectory(rigid_injection)
+add_subdirectory(secondary_ion_emission)
 add_subdirectory(scraping)
 add_subdirectory(effective_potential_electrostatic)
 add_subdirectory(silver_mueller)
diff --git a/Examples/Tests/secondary_ion_emission/CMakeLists.txt b/Examples/Tests/secondary_ion_emission/CMakeLists.txt
new file mode 100644
index 00000000000..e6e38138a08
--- /dev/null
+++ b/Examples/Tests/secondary_ion_emission/CMakeLists.txt
@@ -0,0 +1,14 @@
+# Add tests (alphabetical order) ##############################################
+#
+
+if(WarpX_EB)
+    add_warpx_test(
+        test_rz_secondary_ion_emission_picmi  # name
+        RZ  # dims
+        1  # nprocs
+        inputs_test_rz_secondary_ion_emission_picmi.py  # inputs
+        "analysis.py diags/diag1/"  # analysis
+        "analysis_default_regression.py --path diags/diag1/"  # checksum
+        OFF  # dependency
+    )
+endif()
diff --git a/Examples/Tests/secondary_ion_emission/analysis.py b/Examples/Tests/secondary_ion_emission/analysis.py
new file mode 100644
index 00000000000..7f43b8031b8
--- /dev/null
+++ b/Examples/Tests/secondary_ion_emission/analysis.py
@@ -0,0 +1,62 @@
+#!/usr/bin/env python
+"""
+This script tests the last coordinates of the emitted secondary electrons.
+The EB sphere is centered on O and has a radius of 0.2.
+The proton is initially at: (0,0,-0.25) and moves with a velocity:
+(0.1e6,0,1.5e6) with a time step of dt = 0.000000015.
+The simulation uses a fixed random seed (np.random.seed(10025015))
+to ensure the emission of secodnary electrons.
+An input file inputs_test_rz_secondary_ion_emission_picmi.py is used.
+"""
+
+import sys
+
+import numpy as np
+import yt
+from openpmd_viewer import OpenPMDTimeSeries
+
+yt.funcs.mylog.setLevel(0)
+
+# Open plotfile specified in command line
+filename = sys.argv[1]
+ts = OpenPMDTimeSeries(filename)
+
+it = ts.iterations
+x, y, z = ts.get_particle(["x", "y", "z"], species="electrons", iteration=it[-1])
+print("x", x)
+print("y", y)
+print("z", z)
+# Analytical results calculated
+x_analytic = [0.004028, 0.003193]
+y_analytic = [-0.0001518, -0.0011041]
+z_analytic = [-0.19967, -0.19926]
+
+N_sec_e = np.size(z)  # number of the secondary electrons
+
+assert N_sec_e == 2, (
+    "Test did not pass: for this set up we expect 2 secondary electrons emitted"
+)
+
+tolerance = 1e-3
+
+for i in range(0, N_sec_e):
+    print("\n")
+    print(f"Electron # {i}:")
+    print("NUMERICAL coordinates of the emitted electrons:")
+    print("x=%5.5f, y=%5.5f, z=%5.5f" % (x[i], y[i], z[i]))
+    print("\n")
+    print("ANALYTICAL coordinates of the point of contact:")
+    print("x=%5.5f, y=%5.5f, z=%5.5f" % (x_analytic[i], y_analytic[i], z_analytic[i]))
+
+    diff_x = np.abs((x[i] - x_analytic[i]) / x_analytic[i])
+    diff_y = np.abs((y[i] - y_analytic[i]) / y_analytic[i])
+    diff_z = np.abs((z[i] - z_analytic[i]) / z_analytic[i])
+
+    print("\n")
+    print("percentage error for x = %5.4f %%" % (diff_x * 100))
+    print("percentage error for y = %5.4f %%" % (diff_y * 100))
+    print("percentage error for z = %5.4f %%" % (diff_z * 100))
+
+    assert (diff_x < tolerance) and (diff_y < tolerance) and (diff_z < tolerance), (
+        "Test particle_boundary_interaction did not pass"
+    )
diff --git a/Examples/Tests/secondary_ion_emission/analysis_default_regression.py b/Examples/Tests/secondary_ion_emission/analysis_default_regression.py
new file mode 120000
index 00000000000..d8ce3fca419
--- /dev/null
+++ b/Examples/Tests/secondary_ion_emission/analysis_default_regression.py
@@ -0,0 +1 @@
+../../analysis_default_regression.py
\ No newline at end of file
diff --git a/Examples/Tests/secondary_ion_emission/inputs_test_rz_secondary_ion_emission_picmi.py b/Examples/Tests/secondary_ion_emission/inputs_test_rz_secondary_ion_emission_picmi.py
new file mode 100644
index 00000000000..5849ba4c59e
--- /dev/null
+++ b/Examples/Tests/secondary_ion_emission/inputs_test_rz_secondary_ion_emission_picmi.py
@@ -0,0 +1,255 @@
+#!/usr/bin/env python3
+# --- Input file for secondary-ion emission testing in RZ via callback function.
+import numpy as np
+from scipy.constants import e, elementary_charge, m_e, proton_mass
+
+from pywarpx import callbacks, particle_containers, picmi
+
+##########################
+# numerics parameters
+##########################
+
+dt = 0.000000015
+
+# --- Nb time steps
+Te = 0.0259  # in eV
+dist_th = np.sqrt(Te * elementary_charge / m_e)
+
+max_steps = 3
+diagnostic_interval = 1
+
+# --- grid
+nr = 64
+nz = 64
+
+rmin = 0.0
+rmax = 2
+zmin = -2
+zmax = 2
+delta_H = 0.4
+E_HMax = 250
+
+np.random.seed(10025015)
+##########################
+# numerics components
+##########################
+
+grid = picmi.CylindricalGrid(
+    number_of_cells=[nr, nz],
+    n_azimuthal_modes=1,
+    lower_bound=[rmin, zmin],
+    upper_bound=[rmax, zmax],
+    lower_boundary_conditions=["none", "dirichlet"],
+    upper_boundary_conditions=["dirichlet", "dirichlet"],
+    lower_boundary_conditions_particles=["none", "reflecting"],
+    upper_boundary_conditions_particles=["absorbing", "reflecting"],
+)
+
+solver = picmi.ElectrostaticSolver(
+    grid=grid, method="Multigrid", warpx_absolute_tolerance=1e-7
+)
+
+embedded_boundary = picmi.EmbeddedBoundary(
+    implicit_function="-(x**2+y**2+z**2-radius**2)", radius=0.2
+)
+
+##########################
+# physics components
+##########################
+
+i_dist = picmi.ParticleListDistribution(
+    x=0.0, y=0.0, z=-0.25, ux=0.1e6, uy=0.0, uz=1.50e6, weight=1
+)
+electrons = picmi.Species(
+    particle_type="electron",  # Specify the particle type
+    name="electrons",  # Name of the species
+)
+
+ions = picmi.Species(
+    name="ions",
+    mass=proton_mass,
+    charge=e,
+    initial_distribution=i_dist,
+    warpx_save_particles_at_eb=1,
+)
+
+##########################
+# diagnostics
+##########################
+
+field_diag = picmi.FieldDiagnostic(
+    name="diag1",
+    grid=grid,
+    period=diagnostic_interval,
+    data_list=["Er", "Ez", "phi", "rho"],  # , "rho_electrons"],
+    warpx_format="openpmd",
+)
+
+part_diag = picmi.ParticleDiagnostic(
+    name="diag1",
+    period=diagnostic_interval,
+    species=[ions, electrons],
+    warpx_format="openpmd",
+)
+
+##########################
+# simulation setup
+##########################
+# num_procs = [1, 1]
+# warpx_numprocs=num_procs,
+sim = picmi.Simulation(
+    solver=solver,
+    time_step_size=dt,
+    max_steps=max_steps,
+    warpx_embedded_boundary=embedded_boundary,
+    warpx_amrex_the_arena_is_managed=1,
+)
+
+sim.add_species(
+    electrons,
+    layout=picmi.GriddedLayout(n_macroparticle_per_cell=[0, 0, 0], grid=grid),
+)
+
+sim.add_species(
+    ions,
+    layout=picmi.GriddedLayout(n_macroparticle_per_cell=[10, 1, 1], grid=grid),
+)
+
+sim.add_diagnostic(part_diag)
+sim.add_diagnostic(field_diag)
+
+sim.initialize_inputs()
+sim.initialize_warpx()
+
+##########################
+# python particle data access
+##########################
+
+
+def concat(list_of_arrays):
+    if len(list_of_arrays) == 0:
+        # Return a 1d array of size 0
+        return np.empty(0)
+    else:
+        return np.concatenate(list_of_arrays)
+
+
+def sigma_nascap(energy_kEv, delta_H, E_HMax):
+    """
+    Compute sigma_nascap for each element in the energy array using a loop.
+
+    Parameters:
+    - energy: ndarray or list, energy values in KeV
+    - delta_H: float, parameter for the formula
+    - E_HMax: float, parameter for the formula in KeV
+
+    Returns:
+    - numpy array, computed probability sigma_nascap
+    """
+    sigma_nascap = np.array([])
+    # Loop through each energy value
+    for energy in energy_kEv:
+        if energy > 0.0:
+            sigma = (
+                delta_H
+                * (E_HMax + 1.0)
+                / (E_HMax * 1.0 + energy)
+                * np.sqrt(energy / 1.0)
+            )
+        else:
+            sigma = 0.0
+        sigma_nascap = np.append(sigma_nascap, sigma)
+    return sigma_nascap
+
+
+def secondary_emission():
+    buffer = particle_containers.ParticleBoundaryBufferWrapper()  # boundary buffer
+    # STEP 1: extract the different parameters of the boundary buffer (normal, time, position)
+    lev = 0  # level 0 (no mesh refinement here)
+    n = buffer.get_particle_boundary_buffer_size("ions", "eb")
+    elect_pc = particle_containers.ParticleContainerWrapper("electrons")
+
+    if n != 0:
+        r = concat(buffer.get_particle_boundary_buffer("ions", "eb", "x", lev))
+        theta = concat(buffer.get_particle_boundary_buffer("ions", "eb", "theta", lev))
+        z = concat(buffer.get_particle_boundary_buffer("ions", "eb", "z", lev))
+        x = r * np.cos(theta)  # from RZ coordinates to 3D coordinates
+        y = r * np.sin(theta)
+        ux = concat(buffer.get_particle_boundary_buffer("ions", "eb", "ux", lev))
+        uy = concat(buffer.get_particle_boundary_buffer("ions", "eb", "uy", lev))
+        uz = concat(buffer.get_particle_boundary_buffer("ions", "eb", "uz", lev))
+        w = concat(buffer.get_particle_boundary_buffer("ions", "eb", "w", lev))
+        nx = concat(buffer.get_particle_boundary_buffer("ions", "eb", "nx", lev))
+        ny = concat(buffer.get_particle_boundary_buffer("ions", "eb", "ny", lev))
+        nz = concat(buffer.get_particle_boundary_buffer("ions", "eb", "nz", lev))
+        delta_t = concat(
+            buffer.get_particle_boundary_buffer("ions", "eb", "deltaTimeScraped", lev)
+        )
+        energy_ions = 0.5 * proton_mass * w * (ux**2 + uy**2 + uz**2)
+        energy_ions_in_kEv = energy_ions / (1.602176634e-19 * 1000)
+        sigma_nascap_ions = sigma_nascap(energy_ions_in_kEv, delta_H, E_HMax)
+        # Loop over all ions in the EB buffer
+        for i in range(0, n):
+            sigma = sigma_nascap_ions[i]
+            sigma_int = int(sigma)
+            rn = np.random.uniform(sigma_int, sigma_int + 1 + np.finfo(float).eps)
+            if rn < sigma:
+                Ne_sec = (
+                    sigma_int + 1
+                )  # number of the secondary electrons to be emitted
+                for j in [0, Ne_sec - 1]:
+                    xe = np.array([])
+                    ye = np.array([])
+                    ze = np.array([])
+                    we = np.array([])
+                    delta_te = np.array([])
+                    uxe = np.array([])
+                    uye = np.array([])
+                    uze = np.array([])
+
+                    # Random thermal momenta distribution
+                    ux_th = np.random.normal(0, dist_th)
+                    uy_th = np.random.normal(0, dist_th)
+                    uz_th = np.random.normal(0, dist_th)
+
+                    un_th = nx[i] * ux_th + ny[i] * uy_th + nz[i] * uz_th
+
+                    if un_th < 0:
+                        ux_th_reflect = (
+                            -2 * un_th * nx[i] + ux_th
+                        )  # for a "mirror reflection" u(sym)=-2(u.n)n+u
+                        uy_th_reflect = -2 * un_th * ny[i] + uy_th
+                        uz_th_reflect = -2 * un_th * nz[i] + uz_th
+
+                        uxe = np.append(uxe, ux_th_reflect)
+                        uye = np.append(uye, uy_th_reflect)
+                        uze = np.append(uze, uz_th_reflect)
+                    else:
+                        uxe = np.append(uxe, ux_th)
+                        uye = np.append(uye, uy_th)
+                        uze = np.append(uze, uz_th)
+
+                    xe = np.append(xe, x[i])
+                    ye = np.append(ye, y[i])
+                    ze = np.append(ze, z[i])
+                    we = np.append(we, w[i])
+                    delta_te = np.append(delta_te, delta_t[i])
+
+                    elect_pc.add_particles(
+                        x=xe + (dt - delta_te) * uxe,
+                        y=ye + (dt - delta_te) * uye,
+                        z=ze + (dt - delta_te) * uze,
+                        ux=uxe,
+                        uy=uye,
+                        uz=uze,
+                        w=we,
+                    )
+            buffer.clear_buffer()  # reinitialise the boundary buffer
+
+
+# using the new particle container modified at the last step
+callbacks.installafterstep(secondary_emission)
+##########################
+# simulation run
+##########################
+sim.step(max_steps)  # the whole process is done "max_steps" times
diff --git a/Regression/Checksum/benchmarks_json/test_rz_secondary_ion_emission_picmi.json b/Regression/Checksum/benchmarks_json/test_rz_secondary_ion_emission_picmi.json
new file mode 100644
index 00000000000..92e3b6ec0cc
--- /dev/null
+++ b/Regression/Checksum/benchmarks_json/test_rz_secondary_ion_emission_picmi.json
@@ -0,0 +1,26 @@
+{
+  "electrons": {
+    "particle_momentum_x": 6.863524723051401e-26,
+    "particle_momentum_y": 1.0324224192517369e-25,
+    "particle_momentum_z": 5.621885683115495e-26,
+    "particle_position_x": 0.0072217326490580675,
+    "particle_position_y": 0.001255871169011761,
+    "particle_position_z": 0.39892796754417836,
+    "particle_weight": 2.0
+  },
+  "ions": {
+    "particle_momentum_x": 0.0,
+    "particle_momentum_y": 0.0,
+    "particle_momentum_z": 0.0,
+    "particle_position_x": 0.0,
+    "particle_position_y": 0.0,
+    "particle_position_z": 0.0,
+    "particle_weight": 0.0
+  },
+  "lev=0": {
+    "Er": 3.996898574068735e-08,
+    "Ez": 3.77948124311196e-08,
+    "phi": 2.359076749421693e-08,
+    "rho": 4.6171309216540875e-15
+  }
+}
\ No newline at end of file