Макаров, Дмитрий Николаевич. Неупругие процессы при взаимодействии полей тяжелых ионов и ультракоротких импульсов электромагнитного поля с атомными системами [Электронный ресурс]: автореф. дис. … д-ра физ.-мат. наук: 01.04.02 / Макаров Дмитрий Николаевич; Северный (Арктический) федеральный университет имени М. В. Ломоносова ; науч. консультант В. И. Матвеев. — Электрон. текстовые дан. (1 файл : 913 Кб). — Санкт-Петербург, 2018. — Загл. с титул. экрана. — Электронная версия печатной публикации. — Свободный доступ из сети Интернет (чтение, печать, копирование). — Adobe Acrobat Reader 7.0. — <URL:http://elib.spbstu.ru/dl/2/r18-38.pdf>. — <URL:http://doi.org/10.18720/SPBPU/2/r18-38>.
| Period | Read | Copy | Open | Total | |||
|---|---|---|---|---|---|---|---|
| Year 2018 | Quarter 3 | August | 10 | 0 | 12 | 0 | 22 |
| September | 10 | 0 | 11 | 0 | 21 | ||
| Quarter 4 | October | 8 | 0 | 2 | 0 | 10 | |
| November | 5 | 0 | 6 | 0 | 11 | ||
| December | 5 | 0 | 6 | 0 | 11 | ||
| Year 2019 | Quarter 1 | January | 3 | 0 | 12 | 0 | 15 |
| February | 5 | 0 | 2 | 0 | 7 | ||
| March | 1 | 0 | 1 | 0 | 2 | ||
| Quarter 2 | April | 18 | 0 | 5 | 0 | 23 | |
| May | 12 | 0 | 10 | 0 | 22 | ||
| June | 12 | 0 | 13 | 0 | 25 | ||
| Quarter 3 | July | 13 | 0 | 15 | 0 | 28 | |
| August | 5 | 0 | 3 | 0 | 8 | ||
| September | 1 | 0 | 0 | 0 | 1 | ||
| Quarter 4 | October | 3 | 0 | 4 | 0 | 7 | |
| November | 2 | 0 | 3 | 0 | 5 | ||
| December | 2 | 0 | 3 | 0 | 5 | ||
| Year 2020 | Quarter 1 | January | 1 | 0 | 2 | 0 | 3 |
| February | 2 | 0 | 6 | 0 | 8 | ||
| March | 9 | 0 | 3 | 0 | 12 | ||
| Quarter 2 | April | 6 | 0 | 0 | 0 | 6 | |
| May | 2 | 0 | 1 | 0 | 3 | ||
| June | 1 | 0 | 0 | 0 | 1 | ||
| Quarter 3 | July | 2 | 0 | 0 | 0 | 2 | |
| August | 1 | 0 | 0 | 0 | 1 | ||
| September | 6 | 0 | 0 | 0 | 6 | ||
| Quarter 4 | October | 6 | 0 | 0 | 0 | 6 | |
| November | 2 | 0 | 7 | 0 | 9 | ||
| December | 4 | 0 | 7 | 0 | 11 | ||
| Year 2021 | Quarter 1 | January | 5 | 0 | 6 | 0 | 11 |
| February | 2 | 0 | 2 | 0 | 4 | ||
| March | 3 | 0 | 3 | 0 | 6 | ||
| Quarter 2 | April | 0 | 0 | 0 | 0 | 0 | |
| May | 2 | 0 | 7 | 0 | 9 | ||
| June | 5 | 0 | 6 | 0 | 11 | ||
| Quarter 3 | July | 5 | 0 | 7 | 0 | 12 | |
| August | 7 | 0 | 5 | 0 | 12 | ||
| September | 0 | 0 | 3 | 0 | 3 | ||
| Quarter 4 | October | 5 | 0 | 5 | 0 | 10 | |
| November | 1 | 0 | 3 | 0 | 4 | ||
| December | 1 | 0 | 1 | 0 | 2 | ||
| Year 2022 | Quarter 1 | January | 0 | 0 | 4 | 0 | 4 |
| February | 1 | 0 | 4 | 0 | 5 | ||
| March | 4 | 0 | 6 | 0 | 10 | ||
| Quarter 2 | April | 1 | 0 | 2 | 0 | 3 | |
| May | 2 | 0 | 3 | 0 | 5 | ||
| June | 1 | 0 | 3 | 0 | 4 | ||
| Quarter 3 | July | 8 | 0 | 3 | 0 | 11 | |
| August | 1 | 0 | 7 | 0 | 8 | ||
| September | 2 | 0 | 0 | 0 | 2 | ||
| Quarter 4 | October | 0 | 0 | 1 | 0 | 1 | |
| November | 5 | 0 | 5 | 0 | 10 | ||
| December | 3 | 0 | 8 | 0 | 11 | ||
| Year 2023 | Quarter 1 | January | 4 | 0 | 20 | 0 | 24 |
| February | 3 | 0 | 10 | 0 | 13 | ||
| March | 2 | 0 | 4 | 0 | 6 | ||
| Quarter 2 | April | 1 | 0 | 3 | 0 | 4 | |
| May | 2 | 0 | 7 | 0 | 9 | ||
| June | 0 | 0 | 6 | 0 | 6 | ||
| Quarter 3 | July | 1 | 0 | 1 | 0 | 2 | |
| August | 2 | 0 | 2 | 0 | 4 | ||
| September | 2 | 0 | 4 | 0 | 6 | ||
| Quarter 4 | October | 8 | 0 | 5 | 0 | 13 | |
| November | 2 | 0 | 6 | 0 | 8 | ||
| December | 3 | 0 | 0 | 0 | 3 | ||
| Year 2024 | Quarter 1 | January | 1 | 0 | 2 | 0 | 3 |
| February | 1 | 0 | 5 | 0 | 6 | ||
| March | 1 | 0 | 1 | 0 | 2 | ||
| Quarter 2 | April | 3 | 0 | 6 | 0 | 9 | |
| May | 5 | 0 | 6 | 0 | 11 | ||
| June | 7 | 0 | 6 | 0 | 13 | ||
| Quarter 3 | July | 6 | 0 | 7 | 0 | 13 | |
| August | 2 | 0 | 3 | 0 | 5 | ||
| September | 5 | 0 | 5 | 0 | 10 | ||
| Quarter 4 | October | 7 | 0 | 4 | 0 | 11 | |
| November | 3 | 0 | 5 | 0 | 8 | ||
| December | 0 | 0 | 5 | 0 | 5 | ||
| Year 2025 | Quarter 1 | January | 11 | 0 | 10 | 0 | 21 |
| February | 1 | 0 | 0 | 0 | 1 | ||
| March | 2 | 0 | 2 | 0 | 4 | ||
| Quarter 2 | April | 3 | 0 | 1 | 0 | 4 | |
| May | 3 | 0 | 1 | 0 | 4 | ||
| June | 4 | 0 | 0 | 0 | 4 | ||
| Quarter 3 | July | 4 | 0 | 5 | 0 | 9 | |
| Total | 320 | 0 | 370 | 0 | 690 | ||