A magnetic resonance method involving the generation of high-frequency pulses and magnetic gradients (g x , g y , g z ) for the selective excitation of an object to be examined that is located in an examination volume, wherein N>1 coils having different spatial transmission characteristics σ n ( r ) are used for the excitation by means of N corresponding transmission channels, wherein σ n ( r ) refers to the spatial transmission characteristic of the n th coil, the magnetic resonance method comprising the following steps: - providing a transversal magnetization m ( r , T ) which is described by m r T = iγm 0 exp − T / T 2 exp − iT ω s ∫ 0 T exp t / T 2 exp it ω s b 1 t r exp i k t ⋅ r dt wherein i stands for an imaginary unit, γ stands for a gyromagnetic ratio, m 0 stands for an equilibrium magnetization, t stands for a time, r stands for a position vector, T stands for a duration of a pulse, T 2 stands for a transversal relaxation time, and ω s stands for a shift of the resonance frequency, k(t) is a vector of a k-space trajectory that is given by the magnetic gradients, and wherein b 1 ( t , r ) stands for the superposition of the individual sensitivity-weighted high-frequency pulses b 1, n ( t ) at each location r which is determined by the formula b 1 t r = ∑ n = 1 N σ n r b 1 , n t - determining the high-frequency pulses by means of a signal equation s n ( t ) according to: s n t = ∫ V σ n * r m r exp t / T 2 exp itω s exp − i k T − t ⋅ r d 3 r wherein V stands for an examination volume, and wherein σ n ∗ ( r ) corresponds to the complexly conjugated transmission characteristic of the n th coil, so that the sought high-frequency pulses b 1, n ( t ) of the individual N transmission channels, upon factors, are obtained as: b 1 , n t = s n T − t J t / iγm 0 wherein J ( t ) is a Jacobi determinant that, under the premise of the bijectivity of k ( t ) on the value range of t, yields the dependence of the coordinate transformation between a time parameterization and the k-space parameterization, - exciting the examination volume with the high-frequency pulses, - detecting the measured signal generated by the high-frequency pulses in the examination volume, and - evaluating the measured signal. - providing a transversal magnetization m ( r , T ) which is described by m r T = iγm 0 exp − T / T 2 exp − iT ω s ∫ 0 T exp t / T 2 exp it ω s b 1 t r exp i k t ⋅ r dt wherein i stands for an imaginary unit, γ stands for a gyromagnetic ratio, m 0 stands for an equilibrium magnetization, t stands for a time, r stands for a position vector, T stands for a duration of a pulse, T 2 stands for a transversal relaxation time, and ω s stands for a shift of the resonance frequency, k(t) is a vector of a k-space trajectory that is given by the magnetic gradients, and wherein b 1 ( t , r ) stands for the superposition of the individual sensitivity-weighted high-frequency pulses b 1, n ( t ) at each location r which is determined by the formula b 1 t r = ∑ n = 1 N σ n r b 1 , n t - determining the high-frequency pulses by means of a signal equation s n ( t ) according to: s n t = ∫ V σ n * r m r exp t / T 2 exp itω s exp − i k T − t ⋅ r d 3 r wherein V stands for an examination volume, and wherein σ n ∗ ( r ) corresponds to the complexly conjugated transmission characteristic of the n th coil, so that the sought high-frequency pulses b 1, n ( t ) of the individual N transmission channels, upon factors, are obtained as: b 1 , n t = s n T − t J t / iγm 0 wherein J ( t ) is a Jacobi determinant that, under the premise of the bijectivity of k ( t ) on the value range of t, yields the dependence of the coordinate transformation between a time parameterization and the k-space parameterization, - exciting the examination volume with the high-frequency pulses, - detecting the measured signal generated by the high-frequency pulses in the examination volume, and - evaluating the measured signal. <EOS>