diff --git a/src/deepquantum/photonic/ansatz.py b/src/deepquantum/photonic/ansatz.py
index 4482f054..b684390c 100644
--- a/src/deepquantum/photonic/ansatz.py
+++ b/src/deepquantum/photonic/ansatz.py
@@ -1,7 +1,8 @@
 """Ansatze: various photonic quantum circuits"""
 
 import copy
-from typing import Any
+from itertools import combinations
+from typing import Any, TYPE_CHECKING
 
 import networkx as nx
 import numpy as np
@@ -13,6 +14,9 @@
 from .qmath import sort_dict_fock_basis, takagi
 from .state import FockState
 
+if TYPE_CHECKING:
+    from openfermion import FermionOperator
+
 
 class Clements(QumodeCircuit):
     """Clements circuit."""
@@ -227,3 +231,298 @@ def graph_density(graph: nx.Graph, samples: dict) -> dict:
             samples_[key] = [temp_prob, density]
         sort_samples = sort_dict_fock_basis(samples_, 1)
         return sort_samples
+
+
+class FermionMapBoson:
+    """A class to map molecular Fermionic Hamiltonians to Bosonic Qumode representations.
+
+    This class utilizes OpenFermion and PySCF to perform electronic structure
+    calculations and applies the Dhar-Mandal-Suryanarayana (DMS) mapping to
+    transform the second-quantized Hamiltonian into a Bosonic Fock space.
+    It supports Active Space approximations to reduce the simulation dimensionality.
+
+    Args:
+        config (dict): A configuration dictionary containing the following keys:
+            'geometry' (list): Molecular structure, e.g., [('H', (0,0,0)), ('H', (0,0,0.74))].
+            'basis' (str): Quantum chemistry basis set (e.g., 'sto-3g', '6-31g').
+            'multiplicity' (int): Spin multiplicity (2S + 1). Usually 1 for closed-shell.
+            'charge' (int): Net charge of the molecule.
+            'n_ele' (int): Total number of electrons in the full system.
+            'n_orbit' (int): Total number of spin-orbitals in the full space.
+            'occupied_indices' (list): Indices of spatial orbitals to be frozen (occupied).
+                                        Electrons in these orbitals do not participate in
+                                        excitations but contribute to the energy constant.
+            'active_indices' (list): Indices of spatial orbitals to be treated as active.
+                                       These form the primary Hilbert space for VQE.
+    """
+
+    def __init__(self, config: dict = None) -> None:
+        self.geometry = config['geometry']
+        self.basis = config['basis']
+        self.multiplicity = config['multiplicity']
+        self.charge = config['charge']
+        self.occupied_indices = config['occupied_indices']
+        self.active_indices = config['active_indices']
+        self.n = config['n_ele'] - 2 * len(self.occupied_indices)
+        self.m = 2 * len(self.active_indices)
+
+    def construct_h_fermion(self):
+        from openfermion import get_fermion_operator
+        from openfermion.chem import MolecularData
+        from openfermionpyscf import run_pyscf
+
+        molecule = MolecularData(self.geometry, self.basis, self.multiplicity, self.charge)
+        molecule = run_pyscf(molecule, run_scf=True, run_fci=True)
+        hamiltonian = molecule.get_molecular_hamiltonian(
+            occupied_indices=self.occupied_indices, active_indices=self.active_indices
+        )
+        fermion_op = get_fermion_operator(hamiltonian)
+        h_matrix, basis_f = self.compute_hamiltonian_matrix(fermion_op, self.n, self.m)
+        self.molecule = molecule
+        self.hamiltonian = hamiltonian
+        self.constant = hamiltonian.constant
+        self.fermion_op = fermion_op
+        self.basis_f = basis_f
+        self.h_matrix = h_matrix
+        return h_matrix
+
+    def mapping(self):
+        self.h_fock, self.map_dic = self.get_dms_mapping(self.h_matrix, self.n, self.m)
+        return self.h_fock
+
+    def fci_energy(self):
+        return self.molecule.fci_energy
+
+    @staticmethod
+    def apply_annihilation(state: tuple, k: int):
+        """Apply the annihilation operator :math:`f_k` to a Slater determinant.
+
+        Args:
+            state: An ordered list of occupied orbitals :math:`(p1, ..., pN)` where :math:`p1 < p2 < ... < pN`.
+            k: The index of the orbital to be annihilated.
+
+        """
+        state = list(state)
+
+        if k not in state:
+            return None  # 轨道未被占据，结果为零
+
+        m = state.index(k)  # k 在列表中的位置（0-indexed）
+        sign = (-1) ** m  # 费米子符号
+        new_state = tuple(state[:m] + state[m + 1 :])
+
+        return (new_state, sign)
+
+    @staticmethod
+    def apply_creation(state, k):
+        """Apply the creation operator :math:`f^†_k` to a Slater determinant.
+
+        Args:
+            state: An ordered list of occupied orbitals :math:`(p1, ..., pN)` where :math:`p1 < p2 < ... < pN`.
+            k: The index of the orbital to be created.
+
+        """
+        state = list(state)
+
+        if k in state:
+            return None  # 轨道已被占据，Pauli不相容
+
+        # 找到插入位置（保持有序）
+        n = sum(1 for p in state if p < k)  # k 前面有 n 个轨道
+        sign = (-1) ** n
+        new_state = tuple(sorted(state + [k]))
+
+        return (new_state, sign)
+
+    def matrix_element_one_body(self, bra: tuple, ket: tuple, p: int, q: int):
+        """Calculate the matrix element of a one-body operator: :math:`⟨bra|f^†_p f_q|ket⟩`.
+
+        Args:
+            bra: N-particle Slater determinant (bra state).
+            ket: N-particle Slater determinant (ket state).
+            p: Index of the creation orbital.
+            q: Index of the annihilation orbital.
+        """
+        # Step 1: f_q 作用在 ket 上
+        result = self.apply_annihilation(ket, q)
+        if result is None:
+            return 0.0
+        int1, sign1 = result
+
+        # Step 2: f†_p 作用在中间态上
+        result = self.apply_creation(int1, p)
+        if result is None:
+            return 0.0
+        final_state, sign2 = result
+
+        # Step 3: 计算内积
+        if final_state == bra:
+            return float(sign1 * sign2)
+        else:
+            return 0.0
+
+    def matrix_element_two_body(self, bra: tuple, ket: tuple, p: int, q: int, r: int, s: int):
+        """Calculate the matrix element of a two-body operator: :math:`⟨bra|f†_p f†_q f_r f_s|ket⟩`.
+
+        The operators are applied from right to left: :math:`f_s`, then :math:`f_r`,
+        then :math:`f†_q`, then :math:`f†_p`.
+
+        Args:
+            bra: N-particle Slater determinant (bra state).
+            ket: N-particle Slater determinant (ket state).
+            p: Indices for the creation operators.
+            q: Indices for the creation operators.
+            r: Indices for the annihilation operators.
+            s: Indices for the annihilation operators.
+        """
+        # Step 1: f_s 作用在 ket 上
+        result = self.apply_annihilation(ket, s)
+        if result is None:
+            return 0.0
+        int1, sign_s = result
+
+        # Step 2: f_r 作用在 int1 上
+        result = self.apply_annihilation(int1, r)
+        if result is None:
+            return 0.0
+        int2, sign_r = result
+
+        # Step 3: f†_q 作用在 int2 上
+        result = self.apply_creation(int2, q)
+        if result is None:
+            return 0.0
+        int3, sign_q = result
+
+        # Step 4: f†_p 作用在 int3 上
+        result = self.apply_creation(int3, p)
+        if result is None:
+            return 0.0
+        final_state, sign_p = result
+
+        # Step 5: 计算内积
+        if final_state == bra:
+            return float(sign_p * sign_q * sign_r * sign_s)
+        else:
+            return 0.0
+
+    @staticmethod
+    def extract_integrals(fermion_op: 'FermionOperator'):
+        """Extract one-body integrals :math:`h[p,q]` and two-body integrals :math:`v[p,q,r,s]` from a FermionOperator.
+
+        The FermionOperator format handles terms like:
+            FermionOperator(0.5, '0^ 1')       -> 0.5 * f†_0 f_1
+            FermionOperator(0.25, '0^ 1^ 2 3') -> 0.25 * f†_0 f†_1 f_2 f_3
+
+        Args:
+            fermion_op: The operator object from OpenFermion.
+        """
+        h = {}  # 单体积分
+        v = {}  # 双体积分
+        constant = 0.0
+
+        for term, coeff in fermion_op.terms.items():
+            if len(term) == 0:
+                # 常数项
+                constant += coeff.real
+
+            elif len(term) == 2:
+                # 单体项 f†_p f_q
+                # term = ((p, 1), (q, 0))，其中1=产生，0=湮灭
+                # 确保顺序是：产生算符在前
+
+                # 找产生和湮灭算符
+                creators = [idx for idx, dag in term if dag == 1]
+                annihilators = [idx for idx, dag in term if dag == 0]
+
+                if len(creators) == 1 and len(annihilators) == 1:
+                    p, q = creators[0], annihilators[0]
+                    h[(p, q)] = h.get((p, q), 0.0) + coeff.real
+
+            elif len(term) == 4:
+                # 双体项 f†_p f†_q f_r f_s
+                creators = [idx for idx, dag in term if dag == 1]
+                annihilators = [idx for idx, dag in term if dag == 0]
+
+                if len(creators) == 2 and len(annihilators) == 2:
+                    p, q = creators[0], creators[1]
+                    # 注意：湮灭算符顺序需要与算符定义一致
+                    # OpenFermion 中 f†_p f†_q f_r f_s 的 annihilators 顺序是 r, s
+                    r, s = annihilators[0], annihilators[1]
+                    v[(p, q, r, s)] = v.get((p, q, r, s), 0.0) + coeff.real
+
+        return h, v, constant
+
+    def compute_hamiltonian_matrix(self, fermion_op: 'FermionOperator', n: int, m: int):
+        """Directly compute the Hamiltonian matrix in the n-particle subspace.
+
+        Args:
+            fermion_op: The input OpenFermion Hamiltonian.
+            n: Number of particles (electrons).
+            m: Number of spin-orbitals.
+        """
+        # Step 1: 枚举基矢
+        basis = list(combinations(range(m), n))
+        dim = len(basis)
+
+        # Step 2: 提取积分系数
+        h_integrals, v_integrals, constant = self.extract_integrals(fermion_op)
+
+        # Step 3: 构造矩阵
+        h_matrix = np.zeros((dim, dim), dtype=complex)
+
+        # 常数项：贡献到所有对角元
+        # for i in range(dim):
+        #     h_matrix[i, i] += constant
+
+        # 单体项
+        for (p, q), h_pq in h_integrals.items():
+            if abs(h_pq) < 1e-8:
+                continue
+
+            for j, ket in enumerate(basis):
+                for i, bra in enumerate(basis):
+                    me = self.matrix_element_one_body(bra, ket, p, q)
+                    if me != 0.0:
+                        h_matrix[i, j] += h_pq * me
+
+        # 双体项
+        for (p, q, r, s), v_pqrs in v_integrals.items():
+            if abs(v_pqrs) < 1e-8:
+                continue
+
+            for j, ket in enumerate(basis):
+                for i, bra in enumerate(basis):
+                    me = self.matrix_element_two_body(bra, ket, p, q, r, s)
+                    if me != 0.0:
+                        # h_matrix[i, j] += 0.5 * v_pqrs * me
+                        h_matrix[i, j] += 1 * v_pqrs * me
+
+        return h_matrix.real, basis
+
+    @staticmethod
+    def get_dms_mapping(h_f, n, m):
+        # 1. 生成所有费米子组合 (按升序)
+        f_basis = list(combinations(range(m), n))
+
+        mapping = {}
+        for i, p in enumerate(f_basis):
+            # 注意：p 是有序元组，如 (0, 1)
+            # p[0] 是 p1, p[1] 是 p2...
+            q = [0] * n
+            # 应用公式 (注意索引对应关系)
+            q[n - 1] = p[0]  # q_N = p1
+            for j in range(1, n):  # 处理 q1 到 q_{N-1}
+                # j 从 1 到 N-1 对应公式中的下标
+                # p 数组索引从 0 开始，所以 p_{N-j+1} 对应 p[N-j], p_{N-j} 对应 p[N-j-1]
+                q[j - 1] = p[n - j] - p[n - j - 1] - 1
+
+            mapping[i] = ['F:', p, 'B:', tuple(q)]
+
+        idx = h_f.nonzero()
+        fock_mapping = []
+        for i in range(len(idx[0])):
+            k = idx[0][i]
+            j = idx[1][i]
+            temp = (h_f[k, j].item(), mapping[k][-1], mapping[j][-1])
+            fock_mapping.append(temp)
+        return fock_mapping, mapping