Q.C, Si and Ge have same lattice structure. Why is C insulator while Si and Ge intrinsic semiconductors?
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Band Gap Energy
What is Band Gap Energy? — A First Look
Imagine you have a single atom. Its electrons live in specific, fixed energy levels — like rungs on a ladder. You can't put an electron halfway between two rungs; it's either on one rung or another.
Now bring two atoms close together. Their electron rungs interact and split into two slightly different energies. Bring a billion atoms together — as in a solid crystal — and those original rungs spread into continuous bands of allowed energies, separated by gaps where no electron can exist.
That gap — the forbidden region between two bands — is the band gap.
The Intuition: A Wall Between Two Rooms
Think of the valence band as the ground floor of a building — electrons here are tightly bound to atoms, not free to move. The conduction band is the first floor above — electrons here can roam freely through the crystal, carrying current.
The band gap is the height of the ceiling between these two floors. An electron needs exactly that much energy to jump from the valence band to the conduction band. If you give it less energy, it stays stuck on the ground floor. If you give it exactly the gap energy or more, it can leap up and become a mobile charge carrier.
In a metal, the valence and conduction bands overlap — there is no gap. That's why metals conduct electricity so easily: electrons already have free states available at no energy cost.
The Precise Statement
Band gap energy (Eg) is the minimum energy required to excite an electron from the top of the valence band to the bottom of the conduction band in a solid.
Eg=Econduction band minimum−Evalence band maximum
It is measured in electron volts (eV). One eV is the energy gained by an electron when accelerated through a potential difference of 1 volt — a tiny but convenient unit for atomic-scale energies.
Why Does It Matter?
The band gap determines almost everything about how a material behaves electrically and optically:
| Material type | Typical Eg | Behaviour |
|---|---|---|
| Conductor (metal) | Eg=0 (bands overlap) | Electrons flow freely at room temperature |
| Semiconductor | 0.1 eV<Eg<3 eV | Conducts only when given energy (heat, light) |
| Insulator | Eg>3 eV | Almost no conduction at normal conditions |
A quick rule of thumb: if a material is transparent to visible light, its band gap is larger than about 3.1 eV (the energy of violet light). Diamond (Eg≈5.5 eV) is transparent; silicon (Eg≈1.1 eV) is opaque and shiny.
A Concrete Example: Silicon
Silicon has a band gap of 1.12 eV at room temperature. This means:
- An electron in the valence band needs at least 1.12 eV to jump to the conduction band.
- Visible light photons have energies between 1.8 eV (red) and 3.1 eV (violet). So silicon absorbs most visible light — that's why solar cells are dark. …
Why this formula?
Band Gap Energy: Why the Formula Holds
The band gap energy Eg is the energy difference between the top of the valence band and the bottom of the conduction band in a solid. The key formula is:
Eg=Ec−Ev
where Ec is the minimum energy of the conduction band and Ev is the maximum energy of the valence band.
But why does this simple difference matter? The answer lies in how electrons behave in a crystal.
The Origin of Energy Bands
In an isolated atom, electrons occupy discrete energy levels. When atoms come together to form a solid, their atomic orbitals overlap. According to the Pauli exclusion principle, no two electrons can occupy the same quantum state. So the discrete levels split into a continuum of closely spaced levels — an energy band.
The valence band is formed from the outermost (valence) atomic orbitals. The conduction band is formed from the next higher set of orbitals (typically the empty orbitals above the valence orbitals). Between these bands lies the band gap — a region of forbidden energies where no electron states exist.
Why the Formula Eg=Ec−Ev Is Not Trivial
You might think: "Of course the gap is the difference between the bottom of one band and the top of another." But the real insight is that Ec and Ev are not arbitrary points — they are the extrema of the band structure.
In a periodic crystal, the electron energy E(k) depends on the wavevector k. The valence band has its maximum at some k-point (often at k=0 for direct-gap semiconductors), and the conduction band has its minimum at some k-point. The band gap is:
Eg=minkcEc(kc)−maxkvEv(kv)
This is not just a difference — it's a minimisation over all possible electron momenta.
Why This Difference Determines Conductivity
The band gap controls whether a material is an insulator, semiconductor, or conductor because of the Fermi-Dirac distribution:
f(E)=1+e(E−EF)/kBT1
At absolute zero, all states below the Fermi level EF are filled, and all above are empty. For an intrinsic semiconductor, EF lies in the middle of the band gap. The probability that an electron is thermally excited from the valence band to the conduction band is proportional to e−Eg/2kBT.
The band gap energy Eg appears in the exponent of the carrier concentration formula:
n=p=NcNve−Eg/2kBT
This is why a small change in Eg causes a huge change in conductivity — it's an exponential dependence.
The Physical Meaning of Eg
The band gap is not just a number — it's the minimum energy required to:
- Break a covalent bond in the crystal (creating an electron-hole pair)
- Promote an electron from a bonding state to an antibonding state
- Create a mobile charge carrier
For example, in silicon (Eg=1.12 eV at 300 K), a photon with energy greater than 1.12 eV can be absorbed, exciting an electron from the valence band to the conduction band. This is why silicon is used in solar cells — the band gap matches the solar spectrum. …
Concept: Band Gap Energy — the energy difference between the valence band and the conduction band determines whether a material behaves as an insulator, semiconductor, or conductor.
Reasoning:
- Carbon (diamond), silicon, and germanium all crystallize in the diamond cubic structure, but their band gaps differ significantly due to the strength of covalent bonding and atomic size.
- Carbon has a very small atomic radius and forms extremely strong σ bonds. This leads to a large splitting between bonding (valence) and antibonding (conduction) states, giving a band gap of about 5.4 eV — too large for thermal excitation of electrons at room temperature. …
The band gap energy (Eg) determines whether a material is an insulator or a semiconductor. Diamond (C) has a large Eg≈5.4 eV, making it an insulator, while Si (Eg≈1.1 eV) and Ge (Eg≈0.7 eV) have smaller gaps, allowing thermal excitation of electrons into the conduction band at room temperature.
The key lies in the band gap energy — the energy difference between the top of the valence band and the bottom of the conduction band. Even though C, Si, and Ge all crystallize in the diamond cubic structure (same lattice), their electronic properties differ dramatically because the size of the band gap changes as you go down Group 14.
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Why the band gap changes with atomic number.
As we move from C → Si → Ge, the atomic radius increases and the valence electrons are less tightly bound to the nucleus. The overlap between atomic orbitals in the crystal becomes weaker, and the energy splitting between bonding (valence) and antibonding (conduction) states decreases. This directly reduces the band gap.
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Quantitative comparison of band gaps at room temperature:
Material Band Gap Eg (eV) Classification Diamond (C) ~5.4 Insulator Silicon (Si) ~1.1 Semiconductor Germanium (Ge) ~0.7 Semiconductor -
The thermal energy available at room temperature.
At room temperature, thermal energy can excite some valence electrons across the gap into the conduction band -- but only if the gap is small enough. Diamond's gap (≈5.4 eV) is far too large for any appreciable thermal excitation, so its conduction band stays essentially empty and it behaves as an insulator. Silicon (≈1.1 eV) and germanium (≈0.7 eV) have gaps small enough that a meaningful number of electrons are thermally excited, giving both materials measurable intrinsic conductivity as semiconductors. …
Method: Band Theory of Solids (Energy Band Analysis)
This question is about why the band gap magnitude determines whether a material is an insulator or a semiconductor, even when the crystal structure is identical.
Step 1 – Recall the band structure of diamond cubic crystals
Carbon (diamond), silicon, and germanium all crystallise in the diamond cubic structure. In each case, the valence electrons form a filled valence band and an empty conduction band, separated by a forbidden energy gap — the band gap Eg.
The only difference is the size of this gap.
Step 2 – Compare the band gap values
| Material | Band gap Eg (eV) at 300 K | Classification |
|---|---|---|
| C (diamond) | ~5.4 eV | Insulator |
| Si | ~1.1 eV | Semiconductor |
| Ge | ~0.7 eV | Semiconductor |
The exact numbers vary slightly with temperature, but the order is fixed: Eg(C)≫Eg(Si)>Eg(Ge).
Step 3 – Relate band gap to thermal excitation of electrons
At any non-zero temperature, some electrons in the valence band gain enough thermal energy to jump across the gap into the conduction band -- but only if the gap is small enough for that jump to be likely.
- For diamond (Eg≈5.4 eV), the gap is far too large to be bridged by thermal energy at ordinary temperatures. The conduction band remains essentially empty → no conductivity → insulator.
- For silicon (Eg≈1.1 eV) and germanium (Eg≈0.7 eV), the gap is small enough that a meaningful fraction of electrons can be thermally excited across it. This creates electron–hole pairs, giving intrinsic conductivity → semiconductors.
A larger band gap always means fewer thermally excited carriers at a given temperature -- this is why diamond, silicon and germanium, despite sharing the same crystal structure, fall into completely different conductivity classes as their band gap shrinks down the group.
--- …
The most common mistake here is treating band gap as a fixed number without connecting it to the underlying physics. Let's break down the errors and how to fix them.
Mistake 1: Saying "C has a larger band gap, so it's an insulator" without explaining why the band gap is larger
Students often just state the fact — diamond has a 5.4 eV gap, Si has 1.1 eV, Ge has 0.7 eV — and stop. That's not an answer; it's a restatement of the question. The examiner wants the reason the band gap differs.
How to avoid: Always connect band gap to atomic size and bond strength. For C (diamond), the atoms are small, the covalent bonds are very strong, and the electrons are tightly held. A large energy is needed to break a bond and promote an electron to the conduction band. As you go down Group 14 (Si, Ge), atomic size increases, bonds become weaker, and the band gap shrinks.
Band gap energy is directly proportional to bond strength. Stronger bonds → larger gap → more insulator-like behaviour.
Mistake 2: Confusing "intrinsic semiconductor" with "having a small band gap"
Some students think any material with a band gap less than ~3 eV is automatically a semiconductor. That's not wrong, but it misses the point: diamond's gap is so large (5.4 eV) that at room temperature, virtually no electrons jump the gap. Si and Ge have gaps small enough that thermal energy at 300 K (~0.026 eV) can excite a meaningful number of electrons.
How to avoid: State the rule of thumb plainly: a band gap above roughly 3 eV behaves as an insulator at room temperature; a gap below that, down to a few tenths of an eV, behaves as a semiconductor. For C, Eg≈5.4 eV is well above that threshold, so negligible intrinsic carriers are generated → insulator. For Si (Eg=1.1 eV) and Ge (Eg=0.7 eV), the gap is comfortably below the threshold, so enough electrons are thermally excited to give measurable conductivity.
Do not say "C is an insulator because it has no free electrons." All four have no free electrons at 0 K. The difference is how many are thermally generated at room temperature.
Mistake 3: Forgetting that all three have the same diamond cubic structure
The question explicitly states they have the same lattice structure. Yet some students write answers like "C is an insulator because of its different crystal structure" — that's factually wrong and loses marks.
How to avoid: Acknowledge the identical structure first, then explain that the atomic properties (size, electronegativity, bond energy) cause the band gap difference, not the arrangement of atoms. The structure determines the type of band structure (indirect gap, etc.), but the magnitude of the gap is set by the atoms themselves.
Mistake 4: Using the wrong band gap values or mixing up Si and Ge
Si: 1.1 eV, Ge: 0.7 eV. Some students reverse them or quote 1.4 eV for Si (that's for GaAs, a compound semiconductor). In an exam, wrong numbers mean wrong reasoning.
How to avoid: Memorise the approximate values for the Group 14 elements:
- C (diamond): 5.4 eV
- Si: 1.1 eV
- Ge: 0.7 eV
- (Sn: 0.08 eV — metallic at room temperature)
Mistake 5: Not mentioning temperature dependence …
Showing the 12 most recent of 13 on this concept.
- COMEDK 2026Set 2026-A1 markMCQQ.Pick out the correct statement from the following; (A) The number density of free electrons in the valance band decides the strength of the electric current (B) Valance band is always completely filled, while conduction band is always partially filled (C) The maximum energy required to shift an electron from the conduction band to valance band is called energy band gap (D) In a semiconductor no free electrons are found in the conduction band at 0 K
›Reveal solutionSolution
The key idea is understanding the definitions of valence band, conduction band, band gap, and the behavior of electrons at absolute zero. The correct statement is that in a semiconductor at 0 K, the conduction band contains no free electrons.
The question tests your grasp of basic semiconductor physics — specifically, the structure of energy bands and how electrons populate them. Let’s clarify each concept before evaluating the options.
Concept & Intuition:
In solids, electrons occupy energy bands: the valence band (filled with electrons in their ground state) and the conduction band (empty or partially filled, where electrons can move freely). The band gap is the energy difference between the top of the valence band and the bottom of the conduction band. At absolute zero (0 K), all electrons are in their lowest energy states — in a semiconductor, this means the valence band is completely full and the conduction band is completely empty. No thermal energy is available to excite electrons across the gap.
Now, evaluate each statement:
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Option (A): “The number density of free electrons in the valence band decides the strength of the electric current.”
- Reasoning: Free electrons in the conduction band (not valence band) are the primary charge carriers for current. In the valence band, electrons are bound and cannot move freely unless they leave holes. So this statement is false.
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Option (B): “Valence band is always completely filled, while conduction band is always partially filled.”
- Reasoning: This is not always true. In metals, the conduction band may be partially filled and the valence band may be partially filled or overlapping. In insulators and semiconductors at 0 K, the valence band is full and conduction band empty. The word “always” makes this incorrect.
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Option (C): “The maximum energy required to shift an electron from the conduction band to valence band is called energy band gap.” …
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- COMEDK 2026Set 2026-A1 markMCQQ.What is the minimum wavelength of radiation required to detect a p-n junction diode made of a semiconductor having band gap 3.3 eV . [Planck's constant h=6.6×1034 J.s ] (A) 3300∘A (B) 4800∘A (C) 3750∘A (D) 7500∘A
›Reveal solutionSolution
The minimum detectable wavelength corresponds to the photon energy exactly matching the band gap. Using E=λhc, the wavelength is λ=Ehc≈3750A˚, so option (C) is correct.
The key idea is that a p-n junction diode can detect radiation only if the incoming photons have enough energy to excite electrons across the band gap. The minimum photon energy needed equals the band gap energy Eg=3.3eV. The corresponding wavelength is the maximum wavelength that can be detected — but the question asks for the minimum wavelength of radiation required, which is actually the same threshold: any photon with energy at least Eg works, so the shortest wavelength that still has enough energy is given by E=hc/λ.
- Convert the band gap to joules Since 1eV=1.6×10−19J,
Eg=3.3eV=3.3×1.6×10−19=5.28×10−19J.
- Use the photon energy–wavelength relation The energy of a photon is E=λhc, so
λ=Ehc.
Here h=6.6×10−34J⋅s and c=3×108m/s.
- Plug in the numbers
λ=5.28×10−19(6.6×10−34)(3×108)=5.28×10−191.98×10−25≈3.75×10−7m.
- Convert to angstroms 1A˚=10−10m, so λ=3.75×10−7m=3750A˚. …
- COMEDK 2025Set 2025-A1 markMCQQ.Diamond is considered as an insulator because (A) Diamond has very large forbidden energy gap. (B) Valance band and conduction band of diamond are overlapping X . (C) In the diamond the carbon atoms are held by weak covalent bonds (D) Refractive index of diamond is very low
›Reveal solutionSolution
Diamond is an insulator because its electrons cannot jump from the valence band to the conduction band — the forbidden energy gap is very large (~5.5 eV), so no conduction occurs at ordinary temperatures.
Concept & Intuition
In solid-state physics, materials are classified by their band structure — the arrangement of energy levels that electrons can occupy.
- Conductors have overlapping valence and conduction bands, so electrons move freely.
- Insulators have a large energy gap between the valence band (full of electrons) and the conduction band (empty).
- Semiconductors have a small gap that electrons can cross with a little energy (heat, light).
Diamond is the classic example of an insulator: its carbon atoms are held by strong covalent bonds, and those bonds lock electrons into a full valence band. To conduct electricity, an electron must gain enough energy to jump the gap — but diamond’s gap is huge (~5.5 eV), far larger than thermal energy at room temperature (~0.025 eV). So essentially no electrons make the jump, and diamond does not conduct.
Now let’s examine each option.
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Option (A): Diamond has very large forbidden energy gap.
This is correct. The forbidden gap (band gap) in diamond is about 5.5 eV. For comparison, silicon (a semiconductor) has a gap of 1.1 eV, and insulators typically have gaps > 3 eV. A large gap means that at ordinary temperatures, virtually no electrons are thermally excited into the conduction band — hence no electrical conduction. This is the fundamental reason diamond is an insulator.
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Option (B): Valence band and conduction band of diamond are overlapping.
This is false. Overlapping bands are characteristic of conductors (metals), where electrons can move freely. In diamond, the bands are well separated by the large gap. Overlap would make diamond a conductor, which it is not.
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Option (C): In diamond, the carbon atoms are held by weak covalent bonds. …
- COMEDK 2025Set 2025-A1 markMCQQ.What is the maximum wave length of EM radiation required to move an electron from the valance band to conduction band of a semiconductor? [Given :Energy gap Eg=1.98×10−19 J; Planck's constant h=6.6×10−34Js ] (A) 10−9 m (B) 10−6 m (C) 10−10 m (D) 10−12 m
›Reveal solutionSolution
The maximum wavelength corresponds to the minimum photon energy needed to bridge the band gap. Using E=hc/λ, we find λ≈10−6m, so option (B) is correct.
Concept & Intuition
To promote an electron from the valence band to the conduction band, a photon must supply at least the band-gap energy Eg. The maximum wavelength that can do this is the one whose photon energy exactly equals Eg — any longer wavelength would have lower energy and be insufficient. So we simply set Ephoton=Eg and solve for λ.
Step-by-step solution
- Relate photon energy to wavelength The energy of a photon is
E=λhc
where h=6.6×10−34Js, c=3.0×108m/s, and λ is the wavelength.
- Set photon energy equal to the band gap For the threshold case,
λmaxhc=Eg
so
λmax=Eghc
- Plug in the numbers
λmax=1.98×10−19(6.6×10−34)(3.0×108)
First compute numerator:
6.6×3.0=19.8⇒19.8×10−26=1.98×10−25
Then divide:
λmax=1.98×10−191.98×10−25=10−6m …
- COMEDK 2025Set 2025-M1 markMCQQ.The electrical conductivity of a semiconductor increases when electromagnetic radiation of wavelength shorter than 1.24μ m is incident on it. The band gap (in eV ) for the semiconductor is (A) 1 eV (B) 1.1 eV (C) 2.48 eV (D) 0.7 eV
›Reveal solutionSolution
The band gap energy equals the photon energy at the threshold wavelength; using E=λhc with λ=1.24 μm gives exactly 1.00 eV, so the correct option is (A).
The key idea is that a semiconductor becomes conductive when incident photons have enough energy to excite electrons across the band gap. The threshold wavelength tells us the minimum photon energy that can do this — that energy is the band gap energy. So we just need to convert the given wavelength into energy using the photon energy formula.
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Recall the photon energy–wavelength relation.
The energy of a photon is E=λhc, where h is Planck’s constant, c is the speed of light, and λ is the wavelength. In electron-volts and micrometres, there’s a handy constant: hc≈1240 eV⋅nm. Since 1 μm=1000 nm, we can write hc≈1.24 eV⋅μm.
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Apply the threshold condition.
The problem says conductivity increases for wavelengths shorter than 1.24 μm. That means the threshold wavelength is λmax=1.24 μm. At this wavelength, the photon energy equals the band gap Eg:
Eg=λmaxhc=1.24 μm1.24 eV⋅μm=1.00 eV.
- Interpret the result. …
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- COMEDK 2025Set 2025-M1 markMCQQ.In the energy band diagram of a material shown below, open circles and filled circles denote holes and electrons respectively. The material is a (A) metal (B) insulator (C) n-type semiconductor (D) p-type semiconductor
›Reveal solutionSolution
The material has a finite band gap with electrons in the conduction band and holes in the valence band. Counting carriers, the holes in the valence band outnumber the electrons in the conduction band, so holes are the majority carriers — the hallmark of a p-type semiconductor. The correct option is (D).
The key to this question is reading the energy band diagram — a picture that tells you where the electrons and holes are sitting. In solid-state physics, the conduction band (upper band) is where free electrons roam and conduct current; the valence band (lower band) is where electrons are bound in covalent bonds, and a missing electron leaves a hole (a positive charge carrier). The gap between them, labelled Eg, is the band gap.
Why this approach works:
If you see filled circles (electrons) in the conduction band, that means some electrons have been excited across the gap. If you see open circles (holes) in the valence band, that means some electrons have left behind vacancies. The relative numbers of electrons and holes tell you whether the material is intrinsic (equal numbers), n-type (more electrons), or p-type (more holes). Metals have no band gap (bands overlap), and insulators have a very large gap with no carriers at room temperature.
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Identify the bands and carriers
- The upper rectangle is the conduction band. It contains 2 filled circles → these are electrons.
- The lower rectangle is the valence band. It contains 4 open circles (holes) and 2 filled circles (electrons that remain in the valence band).
- So the material has 2 free electrons in the conduction band and 4 holes in the valence band.
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Interpret the band gap
- The vertical double-headed arrow labelled Eg shows a finite, non-zero band gap. This rules out a metal (which has overlapping bands, i.e., Eg=0).
- The gap is not huge (no numerical value given, but the diagram shows a moderate gap — typical of a semiconductor). An insulator would have a very large Eg and essentially no carriers in the conduction band at ordinary temperatures.
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Compare electron and hole counts
- Electrons in conduction band: 2
- Holes in valence band: 4
- This is not equal — there are more holes than electrons. In an intrinsic (pure) semiconductor, the number of electrons in the conduction band equals the number of holes in the valence band (because each excited electron leaves one hole). Here, the numbers are unequal, so the material is doped.
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Determine the doping type
- In an n-type semiconductor, donor impurities add extra electrons, so the electron concentration n is greater than the hole concentration p. But wait — the diagram shows more holes (4) than electrons (2). That seems backward at first glance. …
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- COMEDK 2024Set 2024-M1 markMCQQ.Though Sn and Si are 4th group elements, Sn is a metal while Si is a semiconductor because (A) Sn has more electrons than Si (B) The energy gap of Sn is zero volt while that of Si is 0.07 V (C) The energy gap of Sn is 1.1 eV volt while that of Si is 0.07 V (D) Sn has more holes than Si
›Reveal solutionSolution
The key idea is that the electrical behavior of an element (metal vs. semiconductor) depends on its band gap energy. Tin (Sn) has a zero band gap, making it a metal, while silicon (Si) has a finite band gap (~1.1 eV), making it a semiconductor. The correct option is (B).
The question asks why Sn and Si, both in Group 14 of the periodic table, behave so differently electrically — Sn is a metal, Si is a semiconductor. The answer lies not in the number of electrons or holes, but in the energy band structure of the solid. In particular, the band gap — the energy difference between the valence band (filled with electrons) and the conduction band (where electrons can move freely) — determines whether a material conducts like a metal, a semiconductor, or an insulator.
- Metals have overlapping bands or a zero band gap, so electrons can move into the conduction band with minimal energy.
- Semiconductors have a small but nonzero band gap (typically 0.1–2 eV), so they conduct only when enough energy (heat, light) is supplied.
- Insulators have a large band gap (>3 eV), so they barely conduct.
Now, let’s examine each option carefully.
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Option (A): "Sn has more electrons than Si"
While it’s true that Sn (atomic number 50) has more electrons than Si (atomic number 14), the number of valence electrons is the same (4 each) because both are in Group 14. The total number of electrons does not determine metallic vs. semiconducting behavior — many elements with many electrons are insulators (e.g., lead is a metal, but bismuth has more electrons and is a semimetal). So this is not the reason.
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Option (B): "The energy gap of Sn is zero volt while that of Si is 0.07 V"
This is almost correct, but the numbers need checking. Actually, the band gap of Si is about 1.1 eV (not 0.07 V). The statement says "0.07 V" for Si, which is wrong. However, the idea that Sn has a zero band gap (or overlapping bands) is correct. In fact, gray tin (the stable form at low temperature) is a semimetal with a very small band gap, but white tin (the common metallic form) has overlapping bands — effectively a zero band gap. So the concept in (B) is right, but the number for Si is incorrect. Still, among the options, this is the only one that points to the band gap difference.
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Option (C): "The energy gap of Sn is 1.1 eV while that of Si is 0.07 V"
This reverses the actual values. Sn does not have a 1.1 eV band gap (it’s essentially zero), and Si’s band gap is ~1.1 eV, not 0.07 eV. So this is completely wrong.
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Option (D): "Sn has more holes than Si" …
- COMEDK 2023Set 2023-E1 markMCQQ.The energy gap between valance band and the conduction band for a given material is 6 eV, then the material is : (A) A semiconductor (B) A metal (C) An insulator (D) A superconductor
›Reveal solutionSolution
An energy gap of 6 eV is far too large for thermal excitation, so the material is an insulator. (Superconductivity is not defined by a band-gap of this kind, so (D) is not the classification asked for.)
Concept: classification of solids by the forbidden-energy-gap Eg between valence and conduction bands.
- Metals (conductors): the bands overlap, Eg is effectively zero.
- Semiconductors: small gap, Eg of the order of ~1 eV (Si 1.1 eV, Ge 0.7 eV), so thermal energy can promote some electrons.
- Insulators: large gap, Eg roughly > 3 eV (e.g. diamond ~ 6 eV); at ordinary temperatures essentially no electron can cross it. …
- COMEDK 2023Set 2023-M1 markMCQQ.An LED is constructed from a p-n junction diode using GaAsP. The energy gap is 1.9 eV. The wavelength of the light emitted will be equal to (A) 10.4×10−26 m (B) 654 nm (C) 654 Ao (D) 654×10−11 m
›Reveal solutionSolution
Using λ=hc/E with hc=1240eV·nm and E=1.9eV gives λ≈654nm (visible red).
The emitted photon energy equals the band gap, E=1.9eV. Its wavelength:
λ=Ehc=1.9 eV1240 eV⋅nm≈653–654 nm. …
- KCET 2022Set B-31 markMCQQ.The forbidden energy gap for ‘Ge’ crystal at ‘0’ K is (A) 1.2 eV (B) 6.57 eV (C) 0.071 eV (D) 0.71 eV
›Reveal solutionSolution
The forbidden energy gap of a germanium crystal at 0 K is a well-known material constant. The correct value is 0.71 eV, which corresponds to option (D).
The forbidden energy gap, or band gap, is the energy difference between the top of the valence band and the bottom of the conduction band in a semiconductor. At absolute zero (0 K), the crystal is in its purest, most ordered state — no thermal energy is available to excite electrons across the gap. For germanium, this intrinsic property is a fixed number, determined by its atomic structure and bonding.
Why does this matter? The band gap dictates whether a material behaves as an insulator, semiconductor, or conductor. For semiconductors like germanium, the gap is small enough that at room temperature, some electrons can jump across, making the material conduct. But at 0 K, the gap is the "true" value, unaltered by thermal expansion or lattice vibrations.
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Recall the known band gaps for common semiconductors.
Silicon (Si) has a band gap of about 1.1 eV at 0 K. Germanium (Ge) has a smaller gap — around 0.67 eV at room temperature, but slightly larger at 0 K due to lattice contraction. The standard accepted value for Ge at 0 K is 0.71 eV.
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Eliminate the distractors.
- Option (A) 1.2 eV is close to silicon’s band gap (1.1 eV), not germanium’s.
- Option (B) 6.57 eV is far too large — that’s in the range of insulators like diamond (5.5 eV).
- Option (C) 0.071 eV is too small; that would make germanium act almost like a conductor at low temperatures, which it doesn’t. …
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- COMEDK 2022Set 20221 markMCQQ.Choose the incorrect statements. (A) Silicon is used in the fabrication of LED. (B) LED works on the principle of electroluminescence. (C) LED is a power efficient device. (D) LED is fabricated with direct band gap semiconductor.
›Reveal solutionSolution
(B) LEDs do work by electroluminescence (radiative recombination of electrons and holes at a forward-biased p-n junction) - CORRECT. (C) LEDs are highly power-efficient (long life, low operating voltage/power) - CORRECT. (D) LEDs are made from DIRECT band-gap semiconductors (GaAs, GaAsP, GaP...) so that recombination gives a photon rather than a phonon - CORRECT. (A) Silicon is an INDIRECT band-gap semiconductor; recombination in Si releases energy mostly as heat (phonons), not light. Silicon is therefore NOT used to fabricate LEDs - this statement is INCORRECT.
Concept: LED physics.
(B) LEDs do work by electroluminescence (radiative recombination of electrons and holes at a forward-biased p-n junction) - CORRECT.
(C) LEDs are highly power-efficient (long life, low operating voltage/power) - CORRECT. …
- COMEDK 2021Set 20211 markMCQQ.What is the minimum band-gap of the LED diode? (A) 1.5 eV (B) 1.7 eV (C) 1.8 eV (D) 0.8 eV
›Reveal solutionSolution
Minimum band gap of an LED = 1.8 eV.
Concept: LED band gap.
For an LED emitting visible light the semiconductor band gap must be at least about the photon energy of red light. NCERT states that LEDs are made of semiconductors with band gap of about 1.8 eV or more (Eg ~ 1.8 eV correspo …
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