Why is the principal energy of an electron lower for excited electrons in a higher energy state? Unicorn Meta Zoo #1: Why another podcast? Announcing the arrival of Valued Associate #679: Cesar Manara 2019 Moderator Election Q&A - Question CollectionEnergy required to remove an electron from HeCan a battery powered by iron and air really provide a feasible power source for automobiles?Calculating the ionization energy for hydrogenLower an electron energy level by pressureIf d-electrons are such poor shielders, why do trends increase more gradually across the d-block than the s or p-block?Wavelength of an electron removed from an atom of hydrogenWhy are higher-energy bonds preferred over lower-energy ones?State symbol for electronIonisation energy is lower for higher energy shell?What is the maximum number of emission lines when the excited electron of a H atom in n = 6 drops to ground state?

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Why is the principal energy of an electron lower for excited electrons in a higher energy state?



Unicorn Meta Zoo #1: Why another podcast?
Announcing the arrival of Valued Associate #679: Cesar Manara
2019 Moderator Election Q&A - Question CollectionEnergy required to remove an electron from HeCan a battery powered by iron and air really provide a feasible power source for automobiles?Calculating the ionization energy for hydrogenLower an electron energy level by pressureIf d-electrons are such poor shielders, why do trends increase more gradually across the d-block than the s or p-block?Wavelength of an electron removed from an atom of hydrogenWhy are higher-energy bonds preferred over lower-energy ones?State symbol for electronIonisation energy is lower for higher energy shell?What is the maximum number of emission lines when the excited electron of a H atom in n = 6 drops to ground state?










8












$begingroup$


Several places state the 'principal energy of an electron' can be calculated as such:



$$E = frac2π^2mZ^2e^4n^2h^2$$



Another equation I found was:



$$E = -fracE_0n^2,$$



where $$E_0 = pu13.6 eV~(pu1 eV = pu1.602e-19 J)$$



As seen in these equations, the greater the principal number ($n$) of the electron, the lower the principal energy $E$ of this electron.



However, the principal number $n$ is associated with higher energy states. The farther from the electron, the higher the energy state of this electron.



I seem to be fumbling the concept of 'principal energy of an electron.' What is the difference between the 'energy state' associated with the principal number, and the 'principal energy' of an electron? What exactly do the 'principal energy' equations mean? I read somewhere that it would be the energy it would take to "unbind" or ionize the electron, which would make sense, but I have not seen 'principal energy' explained as the ionization energy of an electron anywhere else.










share|improve this question











$endgroup$
















    8












    $begingroup$


    Several places state the 'principal energy of an electron' can be calculated as such:



    $$E = frac2π^2mZ^2e^4n^2h^2$$



    Another equation I found was:



    $$E = -fracE_0n^2,$$



    where $$E_0 = pu13.6 eV~(pu1 eV = pu1.602e-19 J)$$



    As seen in these equations, the greater the principal number ($n$) of the electron, the lower the principal energy $E$ of this electron.



    However, the principal number $n$ is associated with higher energy states. The farther from the electron, the higher the energy state of this electron.



    I seem to be fumbling the concept of 'principal energy of an electron.' What is the difference between the 'energy state' associated with the principal number, and the 'principal energy' of an electron? What exactly do the 'principal energy' equations mean? I read somewhere that it would be the energy it would take to "unbind" or ionize the electron, which would make sense, but I have not seen 'principal energy' explained as the ionization energy of an electron anywhere else.










    share|improve this question











    $endgroup$














      8












      8








      8





      $begingroup$


      Several places state the 'principal energy of an electron' can be calculated as such:



      $$E = frac2π^2mZ^2e^4n^2h^2$$



      Another equation I found was:



      $$E = -fracE_0n^2,$$



      where $$E_0 = pu13.6 eV~(pu1 eV = pu1.602e-19 J)$$



      As seen in these equations, the greater the principal number ($n$) of the electron, the lower the principal energy $E$ of this electron.



      However, the principal number $n$ is associated with higher energy states. The farther from the electron, the higher the energy state of this electron.



      I seem to be fumbling the concept of 'principal energy of an electron.' What is the difference between the 'energy state' associated with the principal number, and the 'principal energy' of an electron? What exactly do the 'principal energy' equations mean? I read somewhere that it would be the energy it would take to "unbind" or ionize the electron, which would make sense, but I have not seen 'principal energy' explained as the ionization energy of an electron anywhere else.










      share|improve this question











      $endgroup$




      Several places state the 'principal energy of an electron' can be calculated as such:



      $$E = frac2π^2mZ^2e^4n^2h^2$$



      Another equation I found was:



      $$E = -fracE_0n^2,$$



      where $$E_0 = pu13.6 eV~(pu1 eV = pu1.602e-19 J)$$



      As seen in these equations, the greater the principal number ($n$) of the electron, the lower the principal energy $E$ of this electron.



      However, the principal number $n$ is associated with higher energy states. The farther from the electron, the higher the energy state of this electron.



      I seem to be fumbling the concept of 'principal energy of an electron.' What is the difference between the 'energy state' associated with the principal number, and the 'principal energy' of an electron? What exactly do the 'principal energy' equations mean? I read somewhere that it would be the energy it would take to "unbind" or ionize the electron, which would make sense, but I have not seen 'principal energy' explained as the ionization energy of an electron anywhere else.







      energy electrons






      share|improve this question















      share|improve this question













      share|improve this question




      share|improve this question








      edited Mar 20 at 17:32









      andselisk

      19.8k667128




      19.8k667128










      asked Mar 20 at 16:12









      chompionchompion

      595




      595




















          1 Answer
          1






          active

          oldest

          votes


















          10












          $begingroup$

          Notice that when $n=1$, we have,
          $$
          E=-E_0=-13.6~mathrmeV
          $$

          which is the negative of the energy required to remove an electron from the ground state of a hydrogen atom.



          If we increase $n$ to say $n=2$, then we have,



          $$
          E=-E_0/4=-3.4~mathrmeV
          $$

          which is a larger number than for $n=1$. Don't let the minus sign confuse you.



          This is a very common source of confusion when these equations are seen for the first time. The confusion often stems from the fact that we are free to choose the zero of energy wherever we would like. So, in this case, zero energy corresponds to the case where the electron and nucleus are infinitely separated which is the $nrightarrowinfty$ limit. So, more negative numbers correspond to lower energies and more tightly bound electrons.






          share|improve this answer











          $endgroup$












          • $begingroup$
            My first exposure to this equation was the first, and read the relation between energy and quantum number was inverse. I don't quite see where the minus would come in the 1st equation, but do see it in others. Thank you
            $endgroup$
            – chompion
            Mar 20 at 17:50










          • $begingroup$
            @jheindel your current formulation implies that you need negative amount of energy (i.e. $-E_0$) to ionize a hydrogen atom.
            $endgroup$
            – Ruslan
            Mar 20 at 21:47










          • $begingroup$
            There's a similar thing for gravitational potential energy. If we set the GPE at infinity to zero, then the GPE for finite $r$ is proportional to $frac -1 r$
            $endgroup$
            – Acccumulation
            Mar 20 at 22:26










          • $begingroup$
            @Ruslan currently it says the energy of an electron in a hydrogen atom is $-E_0$ which means the energy required to ionize the hydrogen atom is $+E_0$.
            $endgroup$
            – jheindel
            Mar 21 at 1:20










          • $begingroup$
            Citing your first sentence: "we have, $E=-E_0$ which is the energy required to remove an electron...". So, $E$ is the energy required, and, since $E_0>0$, this energy required is $E<0$.
            $endgroup$
            – Ruslan
            Mar 21 at 4:59











          Your Answer








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          1 Answer
          1






          active

          oldest

          votes








          1 Answer
          1






          active

          oldest

          votes









          active

          oldest

          votes






          active

          oldest

          votes









          10












          $begingroup$

          Notice that when $n=1$, we have,
          $$
          E=-E_0=-13.6~mathrmeV
          $$

          which is the negative of the energy required to remove an electron from the ground state of a hydrogen atom.



          If we increase $n$ to say $n=2$, then we have,



          $$
          E=-E_0/4=-3.4~mathrmeV
          $$

          which is a larger number than for $n=1$. Don't let the minus sign confuse you.



          This is a very common source of confusion when these equations are seen for the first time. The confusion often stems from the fact that we are free to choose the zero of energy wherever we would like. So, in this case, zero energy corresponds to the case where the electron and nucleus are infinitely separated which is the $nrightarrowinfty$ limit. So, more negative numbers correspond to lower energies and more tightly bound electrons.






          share|improve this answer











          $endgroup$












          • $begingroup$
            My first exposure to this equation was the first, and read the relation between energy and quantum number was inverse. I don't quite see where the minus would come in the 1st equation, but do see it in others. Thank you
            $endgroup$
            – chompion
            Mar 20 at 17:50










          • $begingroup$
            @jheindel your current formulation implies that you need negative amount of energy (i.e. $-E_0$) to ionize a hydrogen atom.
            $endgroup$
            – Ruslan
            Mar 20 at 21:47










          • $begingroup$
            There's a similar thing for gravitational potential energy. If we set the GPE at infinity to zero, then the GPE for finite $r$ is proportional to $frac -1 r$
            $endgroup$
            – Acccumulation
            Mar 20 at 22:26










          • $begingroup$
            @Ruslan currently it says the energy of an electron in a hydrogen atom is $-E_0$ which means the energy required to ionize the hydrogen atom is $+E_0$.
            $endgroup$
            – jheindel
            Mar 21 at 1:20










          • $begingroup$
            Citing your first sentence: "we have, $E=-E_0$ which is the energy required to remove an electron...". So, $E$ is the energy required, and, since $E_0>0$, this energy required is $E<0$.
            $endgroup$
            – Ruslan
            Mar 21 at 4:59















          10












          $begingroup$

          Notice that when $n=1$, we have,
          $$
          E=-E_0=-13.6~mathrmeV
          $$

          which is the negative of the energy required to remove an electron from the ground state of a hydrogen atom.



          If we increase $n$ to say $n=2$, then we have,



          $$
          E=-E_0/4=-3.4~mathrmeV
          $$

          which is a larger number than for $n=1$. Don't let the minus sign confuse you.



          This is a very common source of confusion when these equations are seen for the first time. The confusion often stems from the fact that we are free to choose the zero of energy wherever we would like. So, in this case, zero energy corresponds to the case where the electron and nucleus are infinitely separated which is the $nrightarrowinfty$ limit. So, more negative numbers correspond to lower energies and more tightly bound electrons.






          share|improve this answer











          $endgroup$












          • $begingroup$
            My first exposure to this equation was the first, and read the relation between energy and quantum number was inverse. I don't quite see where the minus would come in the 1st equation, but do see it in others. Thank you
            $endgroup$
            – chompion
            Mar 20 at 17:50










          • $begingroup$
            @jheindel your current formulation implies that you need negative amount of energy (i.e. $-E_0$) to ionize a hydrogen atom.
            $endgroup$
            – Ruslan
            Mar 20 at 21:47










          • $begingroup$
            There's a similar thing for gravitational potential energy. If we set the GPE at infinity to zero, then the GPE for finite $r$ is proportional to $frac -1 r$
            $endgroup$
            – Acccumulation
            Mar 20 at 22:26










          • $begingroup$
            @Ruslan currently it says the energy of an electron in a hydrogen atom is $-E_0$ which means the energy required to ionize the hydrogen atom is $+E_0$.
            $endgroup$
            – jheindel
            Mar 21 at 1:20










          • $begingroup$
            Citing your first sentence: "we have, $E=-E_0$ which is the energy required to remove an electron...". So, $E$ is the energy required, and, since $E_0>0$, this energy required is $E<0$.
            $endgroup$
            – Ruslan
            Mar 21 at 4:59













          10












          10








          10





          $begingroup$

          Notice that when $n=1$, we have,
          $$
          E=-E_0=-13.6~mathrmeV
          $$

          which is the negative of the energy required to remove an electron from the ground state of a hydrogen atom.



          If we increase $n$ to say $n=2$, then we have,



          $$
          E=-E_0/4=-3.4~mathrmeV
          $$

          which is a larger number than for $n=1$. Don't let the minus sign confuse you.



          This is a very common source of confusion when these equations are seen for the first time. The confusion often stems from the fact that we are free to choose the zero of energy wherever we would like. So, in this case, zero energy corresponds to the case where the electron and nucleus are infinitely separated which is the $nrightarrowinfty$ limit. So, more negative numbers correspond to lower energies and more tightly bound electrons.






          share|improve this answer











          $endgroup$



          Notice that when $n=1$, we have,
          $$
          E=-E_0=-13.6~mathrmeV
          $$

          which is the negative of the energy required to remove an electron from the ground state of a hydrogen atom.



          If we increase $n$ to say $n=2$, then we have,



          $$
          E=-E_0/4=-3.4~mathrmeV
          $$

          which is a larger number than for $n=1$. Don't let the minus sign confuse you.



          This is a very common source of confusion when these equations are seen for the first time. The confusion often stems from the fact that we are free to choose the zero of energy wherever we would like. So, in this case, zero energy corresponds to the case where the electron and nucleus are infinitely separated which is the $nrightarrowinfty$ limit. So, more negative numbers correspond to lower energies and more tightly bound electrons.







          share|improve this answer














          share|improve this answer



          share|improve this answer








          edited Mar 21 at 6:24

























          answered Mar 20 at 17:32









          jheindeljheindel

          8,2742655




          8,2742655











          • $begingroup$
            My first exposure to this equation was the first, and read the relation between energy and quantum number was inverse. I don't quite see where the minus would come in the 1st equation, but do see it in others. Thank you
            $endgroup$
            – chompion
            Mar 20 at 17:50










          • $begingroup$
            @jheindel your current formulation implies that you need negative amount of energy (i.e. $-E_0$) to ionize a hydrogen atom.
            $endgroup$
            – Ruslan
            Mar 20 at 21:47










          • $begingroup$
            There's a similar thing for gravitational potential energy. If we set the GPE at infinity to zero, then the GPE for finite $r$ is proportional to $frac -1 r$
            $endgroup$
            – Acccumulation
            Mar 20 at 22:26










          • $begingroup$
            @Ruslan currently it says the energy of an electron in a hydrogen atom is $-E_0$ which means the energy required to ionize the hydrogen atom is $+E_0$.
            $endgroup$
            – jheindel
            Mar 21 at 1:20










          • $begingroup$
            Citing your first sentence: "we have, $E=-E_0$ which is the energy required to remove an electron...". So, $E$ is the energy required, and, since $E_0>0$, this energy required is $E<0$.
            $endgroup$
            – Ruslan
            Mar 21 at 4:59
















          • $begingroup$
            My first exposure to this equation was the first, and read the relation between energy and quantum number was inverse. I don't quite see where the minus would come in the 1st equation, but do see it in others. Thank you
            $endgroup$
            – chompion
            Mar 20 at 17:50










          • $begingroup$
            @jheindel your current formulation implies that you need negative amount of energy (i.e. $-E_0$) to ionize a hydrogen atom.
            $endgroup$
            – Ruslan
            Mar 20 at 21:47










          • $begingroup$
            There's a similar thing for gravitational potential energy. If we set the GPE at infinity to zero, then the GPE for finite $r$ is proportional to $frac -1 r$
            $endgroup$
            – Acccumulation
            Mar 20 at 22:26










          • $begingroup$
            @Ruslan currently it says the energy of an electron in a hydrogen atom is $-E_0$ which means the energy required to ionize the hydrogen atom is $+E_0$.
            $endgroup$
            – jheindel
            Mar 21 at 1:20










          • $begingroup$
            Citing your first sentence: "we have, $E=-E_0$ which is the energy required to remove an electron...". So, $E$ is the energy required, and, since $E_0>0$, this energy required is $E<0$.
            $endgroup$
            – Ruslan
            Mar 21 at 4:59















          $begingroup$
          My first exposure to this equation was the first, and read the relation between energy and quantum number was inverse. I don't quite see where the minus would come in the 1st equation, but do see it in others. Thank you
          $endgroup$
          – chompion
          Mar 20 at 17:50




          $begingroup$
          My first exposure to this equation was the first, and read the relation between energy and quantum number was inverse. I don't quite see where the minus would come in the 1st equation, but do see it in others. Thank you
          $endgroup$
          – chompion
          Mar 20 at 17:50












          $begingroup$
          @jheindel your current formulation implies that you need negative amount of energy (i.e. $-E_0$) to ionize a hydrogen atom.
          $endgroup$
          – Ruslan
          Mar 20 at 21:47




          $begingroup$
          @jheindel your current formulation implies that you need negative amount of energy (i.e. $-E_0$) to ionize a hydrogen atom.
          $endgroup$
          – Ruslan
          Mar 20 at 21:47












          $begingroup$
          There's a similar thing for gravitational potential energy. If we set the GPE at infinity to zero, then the GPE for finite $r$ is proportional to $frac -1 r$
          $endgroup$
          – Acccumulation
          Mar 20 at 22:26




          $begingroup$
          There's a similar thing for gravitational potential energy. If we set the GPE at infinity to zero, then the GPE for finite $r$ is proportional to $frac -1 r$
          $endgroup$
          – Acccumulation
          Mar 20 at 22:26












          $begingroup$
          @Ruslan currently it says the energy of an electron in a hydrogen atom is $-E_0$ which means the energy required to ionize the hydrogen atom is $+E_0$.
          $endgroup$
          – jheindel
          Mar 21 at 1:20




          $begingroup$
          @Ruslan currently it says the energy of an electron in a hydrogen atom is $-E_0$ which means the energy required to ionize the hydrogen atom is $+E_0$.
          $endgroup$
          – jheindel
          Mar 21 at 1:20












          $begingroup$
          Citing your first sentence: "we have, $E=-E_0$ which is the energy required to remove an electron...". So, $E$ is the energy required, and, since $E_0>0$, this energy required is $E<0$.
          $endgroup$
          – Ruslan
          Mar 21 at 4:59




          $begingroup$
          Citing your first sentence: "we have, $E=-E_0$ which is the energy required to remove an electron...". So, $E$ is the energy required, and, since $E_0>0$, this energy required is $E<0$.
          $endgroup$
          – Ruslan
          Mar 21 at 4:59

















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          Старые Смолеговицы Содержание История | География | Демография | Достопримечательности | Примечания | НавигацияHGЯOLHGЯOL41 206 832 01641 606 406 141Административно-территориальное деление Ленинградской области«Переписная оброчная книга Водской пятины 1500 года», С. 793«Карта Ингерманландии: Ивангорода, Яма, Копорья, Нотеборга», по материалам 1676 г.«Генеральная карта провинции Ингерманландии» Э. Белинга и А. Андерсина, 1704 г., составлена по материалам 1678 г.«Географический чертёж над Ижорскою землей со своими городами» Адриана Шонбека 1705 г.Новая и достоверная всей Ингерманландии ланткарта. Грав. А. Ростовцев. СПб., 1727 г.Топографическая карта Санкт-Петербургской губернии. 5-и верстка. Шуберт. 1834 г.Описание Санкт-Петербургской губернии по уездам и станамСпецкарта западной части России Ф. Ф. Шуберта. 1844 г.Алфавитный список селений по уездам и станам С.-Петербургской губернииСписки населённых мест Российской Империи, составленные и издаваемые центральным статистическим комитетом министерства внутренних дел. XXXVII. Санкт-Петербургская губерния. По состоянию на 1862 год. СПб. 1864. С. 203Материалы по статистике народного хозяйства в С.-Петербургской губернии. Вып. IX. Частновладельческое хозяйство в Ямбургском уезде. СПб, 1888, С. 146, С. 2, 7, 54Положение о гербе муниципального образования Курское сельское поселениеСправочник истории административно-территориального деления Ленинградской области.Топографическая карта Ленинградской области, квадрат О-35-23-В (Хотыницы), 1930 г.АрхивированоАдминистративно-территориальное деление Ленинградской области. — Л., 1933, С. 27, 198АрхивированоАдминистративно-экономический справочник по Ленинградской области. — Л., 1936, с. 219АрхивированоАдминистративно-территориальное деление Ленинградской области. — Л., 1966, с. 175АрхивированоАдминистративно-территориальное деление Ленинградской области. — Лениздат, 1973, С. 180АрхивированоАдминистративно-территориальное деление Ленинградской области. — Лениздат, 1990, ISBN 5-289-00612-5, С. 38АрхивированоАдминистративно-территориальное деление Ленинградской области. — СПб., 2007, с. 60АрхивированоКоряков Юрий База данных «Этно-языковой состав населённых пунктов России». Ленинградская область.Административно-территориальное деление Ленинградской области. — СПб, 1997, ISBN 5-86153-055-6, С. 41АрхивированоКультовый комплекс Старые Смолеговицы // Электронная энциклопедия ЭрмитажаПроблемы выявления, изучения и сохранения культовых комплексов с каменными крестами: по материалам работ 2016-2017 гг. в Ленинградской области