Ordered by composite index (descending). Higher values indicate more intensive citation.
| # | Reference | Year | Mentions | Breadth | Sec. Wtd | Share | Composite | Main % |
|---|---|---|---|---|---|---|---|---|
| 1 | Chernozhukov, Lee and Rosen (self) | 2013 | 4 | 3 | 3.0 | 0.046 | 0.928 | 100% |
| 2 | Manski | 2021 | 5 | 2 | 4.0 | 0.057 | 0.874 | 100% |
| 3 | Kitagawa and Tetenov | 2018 | 4 | 2 | 3.5 | 0.046 | 0.811 | 100% |
| 4 | Athey and Wager | 2021 | 4 | 2 | 5.0 | 0.046 | 0.811 | 100% |
| 5 | Andrews and Chen | 2025 | 4 | 2 | 2.5 | 0.046 | 0.811 | 100% |
| 6 | Ben-Michael, Greiner, Imai and Jiang | 2025 | 3 | 2 | 2.0 | 0.034 | 0.737 | 100% |
| 7 | Andrews, Kitagawa and McCloskey | 2024 | 2 | 2 | 1.5 | 0.023 | 0.644 | 100% |
| 8 | Hendren and Sprung-Keyser | 2021 | 2 | 2 | 3.0 | 0.023 | 0.644 | 100% |
| 9 | Chernozhukov, Chetverikov, Kato and Koike (self) | 2022 | 2 | 2 | 4.0 | 0.023 | 0.644 | 100% |
| 10 | Chernozhukov, Chetverikov and Koike (self) | 2023 | 2 | 2 | 4.0 | 0.023 | 0.644 | 100% |
| 11 | Chernozhukov, Chetverikov, Kato and Koike (self) | 2023 | 2 | 2 | 4.0 | 0.023 | 0.644 | 100% |
| 12 | Belloni, Chernozhukov, Chetverikov and Wei (self) | 2018 | 2 | 2 | 4.0 | 0.023 | 0.644 | 100% |
| 13 | Quintas-Martinez | 2022 | 2 | 2 | 4.0 | 0.023 | 0.644 | 100% |
| 14 | Hendren and Sprung-Keyser | 2020 | 2 | 1 | 2.0 | 0.023 | 0.511 | 100% |
| 15 | Sun (self) | 2025 | 2 | 1 | 1.0 | 0.023 | 0.511 | 100% |
| 16 | Moon | 2025 | 2 | 1 | 1.0 | 0.023 | 0.511 | 100% |
| 17 | Hendren | 2020 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 18 | Garc\'\ia and Heckman | 2022 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 19 | Salisbury | 2024 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 20 | Wald | 1950 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 21 | Manski | 2004 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 22 | Dehejia | 2005 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 23 | Stoye | 2009 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 24 | Hirano and Porter | 2009 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 25 | Hirano and Porter | 2020 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 26 | Manski | 2023 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 27 | Mbakop and Tabord-Meehan | 2021 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 28 | Demirer, Syrgkanis, Lewis and Chernozhukov (self) | 2019 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 29 | Belloni, Chernozhukov, Chetverikov, Hansen and Kat... (self) | 2018 | 1 | 1 | 2.0 | 0.011 | 0.406 | 100% |
| 30 | Maurer and Pontil | 2009 | 1 | 1 | 2.0 | 0.011 | 0.406 | 100% |
| 31 | Swaminathan and Joachims | 2015 | 1 | 1 | 2.0 | 0.011 | 0.406 | 100% |
| 32 | Foster and Syrgkanis | 2023 | 1 | 1 | 2.0 | 0.011 | 0.406 | 100% |
| 33 | Kiyani, Pappas, Roth and Hassani | 2025 | 1 | 1 | 0.5 | 0.011 | 0.406 | 100% |
| 34 | Benjamini, Hechtlinger and Stark | 2019 | 1 | 1 | 0.5 | 0.011 | 0.406 | 100% |
| 35 | Zrnic and Fithian | 2024 | 1 | 1 | 0.5 | 0.011 | 0.406 | 100% |
| 36 | Zrnic and Fithian | 2025 | 1 | 1 | 0.5 | 0.011 | 0.406 | 100% |
| 37 | Rai | 2019 | 1 | 1 | 0.5 | 0.011 | 0.406 | 100% |
| 38 | Armstrong and Shen | 2023 | 1 | 1 | 0.5 | 0.011 | 0.406 | 100% |
| 39 | Ponomarev and Semenova | 2024 | 1 | 1 | 0.5 | 0.011 | 0.406 | 100% |
| 40 | Manski | 2019 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 41 | Manski | 2000 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 42 | Russell | 2020 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 43 | Ishihara and Kitagawa | 2021 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 44 | Yata | 2021 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 45 | Christensen, Moon and Schorfheide | 2023 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 46 | Kido | 2023 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 47 | Montiel Olea, Qiu and Stoye | 2025 | 1 | 1 | 1.0 | 0.011 | 0.406 | 100% |
| 48 | Banerjee, Chandrasekhar, Dalpath, Duflo, Floretta,... | 2025 | 4 | 2 | 2.0 | 0.046 | 0.175 | 0% |
| 49 | Schilbach | 2019 | 3 | 2 | 1.5 | 0.034 | 0.159 | 0% |
| 50 | Dupas and Robinson | 2013 | 2 | 2 | 1.0 | 0.023 | 0.139 | 0% |
| 51 | Doksum and Lo | 1990 | 1 | 1 | 0.5 | 0.011 | 0.087 | 0% |
| 52 | Liese and Miescke | 2008 | 1 | 1 | 0.5 | 0.011 | 0.087 | 0% |
| 53 | Newey | 1994 | 1 | 1 | 0.5 | 0.011 | 0.087 | 0% |