/** * @license * Copyright 2020 Google LLC. All Rights Reserved. * Licensed under the Apache License, Version 2.0 (the "License"); * you may not use this file except in compliance with the License. * You may obtain a copy of the License at * * http://www.apache.org/licenses/LICENSE-2.0 * * Unless required by applicable law or agreed to in writing, software * distributed under the License is distributed on an "AS IS" BASIS, * WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. * See the License for the specific language governing permissions and * limitations under the License. * ============================================================================= */ import { ENGINE } from '../engine'; import { Real } from '../kernel_names'; import { convertToTensor } from '../tensor_util_env'; import { op } from './operation'; /** * Returns the real part of a complex (or real) tensor. * * Given a tensor input, this operation returns a tensor of type float that is * the real part of each element in input considered as a complex number. * * If the input is real, it simply makes a clone. * * ```js * const x = tf.complex([-2.25, 3.25], [4.75, 5.75]); * tf.real(x).print(); * ``` * * @doc {heading: 'Tensors', subheading: 'Creation'} */ function real_(input) { const $input = convertToTensor(input, 'input', 'real'); const inputs = { input: $input }; return ENGINE.runKernel(Real, inputs); } export const real = /* @__PURE__ */ op({ real_ }); //# sourceMappingURL=data:application/json;base64,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