We continue our study of string theory in a background that interpolates between <math><mi>A</mi><mi>d</mi><msub><mrow><mi>S</mi></mrow><mrow><mn>3</mn></mrow></msub></math> in the infrared and a linear dilaton spacetime <math><msup><mrow><mi>IR</mi></mrow><mrow><mn>1</mn><mo>,</mo><mn>1</mn></mrow></msup><mo>×</mo><msub><mrow><mi>IR</mi></mrow><mrow><mi>ϕ</mi></mrow></msub></math> in the UV. This background corresponds via holography to a <math><mi>C</mi><mi>F</mi><msub><mrow><mi>T</mi></mrow><mrow><mn>2</mn></mrow></msub></math> deformed by an operator of dimension <math><mo>(</mo><mn>2</mn><mo>,</mo><mn>2</mn><mo>)</mo></math>. We discuss the structure of spatial entanglement in this model, and compare it to the closely related <math><mi>T</mi><mover><mrow><mi>T</mi></mrow><mo>‾</mo></mover></math> deformed <math><mi>C</mi><mi>F</mi><msub><mrow><mi>T</mi></mrow><mrow><mn>2</mn></mrow></msub></math>.