/** * @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 { Identity } from '../kernel_names'; import { convertToTensor } from '../tensor_util_env'; import { op } from './operation'; /** * Creates a new tensor with the same values and shape as the specified * tensor. * * ```js * const x = tf.tensor([1, 2]); * * x.clone().print(); * ``` * * @param x The tensor to clone. * * @doc {heading: 'Tensors', subheading: 'Creation'} */ function clone_(x) { const $x = convertToTensor(x, 'x', 'clone', 'string_or_numeric'); const inputs = { x: $x }; // Note this op is called tf.identity in python. Hence the kernel name used // here. return ENGINE.runKernel(Identity, inputs); } export const clone = /* @__PURE__ */ op({ clone_ }); //# sourceMappingURL=data:application/json;base64,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