/** * @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 { convertToTensor } from '../tensor_util_env'; import { squeezeShape } from '../util'; import { op } from './operation'; import { reshape } from './reshape'; /** * Removes dimensions of size 1 from the shape of a `tf.Tensor`. * * ```js * const x = tf.tensor([1, 2, 3, 4], [1, 1, 4]); * x.squeeze().print(); * ``` * * @param x The input tensor to be squeezed. * @param axis An optional list of numbers. If specified, only * squeezes the dimensions listed. The dimension index starts at 0. It * is an error to squeeze a dimension that is not 1. * * @doc {heading: 'Tensors', subheading: 'Transformations'} */ function squeeze_(x, axis) { const $x = convertToTensor(x, 'x', 'squeeze', 'string_or_numeric'); return reshape($x, squeezeShape($x.shape, axis).newShape); } export const squeeze = /* @__PURE__ */ op({ squeeze_ }); //# sourceMappingURL=data:application/json;base64,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