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I am confused on a topic regarding NPN BJT transistors. enter image description here

When there is a collector-emitter voltage (VCE) applied to the NPN transistor (as shown in the figure) without a emitter-base voltage (VBE), it is said that this forward biases the emitter-base junction (J1) and reverse biases the base-collector junction (J2). My confusion arises when J1 is said to be forward biased, does this mean the depletion region at J1 is reducing in size since the collector is at a lower potential and electrons are entering the depletion region due to the negative terminal of the battery. When I think of forward biasing a PN junction, the depletion region reduces until it fully 'disappears' at 0.7V (for silicon). If the depletion region is slowly decreasing, doesn't this mean some electrons can enter into the P base region?

Apologies for the simple question, just slightly confused.

Thanks

Edit: Where I have written 'it is said', I am referring to Fundamentals of Power Semiconductor Devices page 528 by Baliga.

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    \$\begingroup\$ Can you draw out the charge density curve for the NPN without the battery? Also, draw out the electric field intensity curve? These help a lot in thinking about what happens when you apply an external field. \$\endgroup\$
    – jonk
    Feb 21, 2022 at 21:25
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    \$\begingroup\$ "it is said". Who said that? Please edit your question to include a link to a web page, or a book. \$\endgroup\$
    – TimWescott
    Feb 22, 2022 at 1:10
  • \$\begingroup\$ I have added the reference to the post \$\endgroup\$
    – Umar
    Feb 22, 2022 at 3:42
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    \$\begingroup\$ "reverse biases the emitter-collector junction" - hard to believe it says that. \$\endgroup\$
    – Finbarr
    Feb 22, 2022 at 9:06
  • \$\begingroup\$ Sorry that was a typo, I meant to say base-collector \$\endgroup\$
    – Umar
    Feb 22, 2022 at 15:46

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When you apply a voltage across the emitter and collector, you are creating an electric field across the entire length of the transistor. Since this electric field is in opposition to the built-in field in the base-emitter junction, it reduces the amount of drift and the depletion region narrows. The opposite is true at the base-collector junction.

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