Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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48163 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.7056 | 0.8857 | 0.7967 | [M:[0.9833, 0.9833, 1.1185, 0.7796, 0.7796, 0.6778], q:[0.576, 0.4407], qb:[0.4407, 0.7796], phi:[0.4407]] | [M:[[1, -7], [-1, -11], [0, 4], [1, 3], [-1, -1], [0, 6]], q:[[0, 11], [-1, -4]], qb:[[1, 0], [0, 1]], phi:[[0, -2]]] |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{6}$, ${ }M_{5}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{4}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}^{2}$ | ${}M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ | -2 | t^2.033 + 2*t^2.339 + t^2.644 + 2*t^2.95 + t^3.356 + 2*t^3.967 + 2*t^4.067 + 4*t^4.372 + 4*t^4.678 + t^4.778 + 4*t^4.983 + 5*t^5.289 + t^5.389 + 2*t^5.695 + 3*t^5.9 - 2*t^6. + 2*t^6.1 + 4*t^6.305 + 4*t^6.406 + t^6.611 + 8*t^6.711 + t^6.812 + 2*t^6.916 + 8*t^7.017 + 2*t^7.117 + 7*t^7.322 + 2*t^7.423 + 6*t^7.628 + 2*t^7.728 + 6*t^7.933 - t^8.033 + 3*t^8.134 + 6*t^8.239 - 4*t^8.339 + 4*t^8.439 + 3*t^8.644 + 8*t^8.745 + 2*t^8.845 + 4*t^8.85 - 6*t^8.95 - t^4.322/y - t^6.356/y - (2*t^6.661)/y - (2*t^7.272)/y + (4*t^7.372)/y + (2*t^7.678)/y + (6*t^7.983)/y + (5*t^8.289)/y + (2*t^8.594)/y + t^8.9/y - t^4.322*y - t^6.356*y - 2*t^6.661*y - 2*t^7.272*y + 4*t^7.372*y + 2*t^7.678*y + 6*t^7.983*y + 5*t^8.289*y + 2*t^8.594*y + t^8.9*y | g2^6*t^2.033 + t^2.339/(g1*g2) + g1*g2^3*t^2.339 + t^2.644/g2^4 + t^2.95/(g1*g2^11) + (g1*t^2.95)/g2^7 + g2^4*t^3.356 + t^3.967/(g1^2*g2^10) + (g1^2*t^3.967)/g2^2 + 2*g2^12*t^4.067 + (2*g2^5*t^4.372)/g1 + 2*g1*g2^9*t^4.372 + t^4.678/(g1^2*g2^2) + 2*g2^2*t^4.678 + g1^2*g2^6*t^4.678 + g2^20*t^4.778 + (2*t^4.983)/(g1*g2^5) + (2*g1*t^4.983)/g2 + t^5.289/(g1^2*g2^12) + (3*t^5.289)/g2^8 + (g1^2*t^5.289)/g2^4 + g2^10*t^5.389 + (g2^3*t^5.695)/g1 + g1*g2^7*t^5.695 + t^5.9/(g1^2*g2^22) + t^5.9/g2^18 + (g1^2*t^5.9)/g2^14 - 2*t^6. + 2*g2^18*t^6.1 + t^6.305/(g1^3*g2^11) + t^6.305/(g1*g2^7) + (g1*t^6.305)/g2^3 + g1^3*g2*t^6.305 + (2*g2^11*t^6.406)/g1 + 2*g1*g2^15*t^6.406 + t^6.611/(g1^2*g2^14) - t^6.611/g2^10 + (g1^2*t^6.611)/g2^6 + (2*g2^4*t^6.711)/g1^2 + 4*g2^8*t^6.711 + 2*g1^2*g2^12*t^6.711 + g2^26*t^6.812 + t^6.916/(g1^3*g2^21) + (g1^3*t^6.916)/g2^9 + t^7.017/(g1^3*g2^3) + (3*g2*t^7.017)/g1 + 3*g1*g2^5*t^7.017 + g1^3*g2^9*t^7.017 + (g2^19*t^7.117)/g1 + g1*g2^23*t^7.117 + (2*t^7.322)/(g1^2*g2^6) + (3*t^7.322)/g2^2 + 2*g1^2*g2^2*t^7.322 + 2*g2^16*t^7.423 + t^7.628/(g1^3*g2^13) + (2*t^7.628)/(g1*g2^9) + (2*g1*t^7.628)/g2^5 + (g1^3*t^7.628)/g2 + (g2^9*t^7.728)/g1 + g1*g2^13*t^7.728 + t^7.933/(g1^4*g2^20) + t^7.933/(g1^2*g2^16) + (2*t^7.933)/g2^12 + (g1^2*t^7.933)/g2^8 + (g1^4*t^7.933)/g2^4 + (g2^2*t^8.033)/g1^2 - 3*g2^6*t^8.033 + g1^2*g2^10*t^8.033 + 3*g2^24*t^8.134 + t^8.239/(g1^3*g2^23) + (2*t^8.239)/(g1*g2^19) + (2*g1*t^8.239)/g2^15 + (g1^3*t^8.239)/g2^11 + t^8.339/(g1^3*g2^5) - (3*t^8.339)/(g1*g2) - 3*g1*g2^3*t^8.339 + g1^3*g2^7*t^8.339 + (2*g2^17*t^8.439)/g1 + 2*g1*g2^21*t^8.439 + g1^2*t^8.644 + t^8.644/(g1^4*g2^12) + t^8.644/(g1^2*g2^8) - t^8.644/g2^4 + g1^4*g2^4*t^8.644 + (3*g2^10*t^8.745)/g1^2 + 2*g2^14*t^8.745 + 3*g1^2*g2^18*t^8.745 + 2*g2^32*t^8.845 + t^8.85/(g1^3*g2^33) + t^8.85/(g1*g2^29) + (g1*t^8.85)/g2^25 + (g1^3*t^8.85)/g2^21 + t^8.95/(g1^3*g2^15) - (4*t^8.95)/(g1*g2^11) - (4*g1*t^8.95)/g2^7 + (g1^3*t^8.95)/g2^3 - t^4.322/(g2^2*y) - (g2^4*t^6.356)/y - t^6.661/(g1*g2^3*y) - (g1*g2*t^6.661)/y - t^7.272/(g1*g2^13*y) - (g1*t^7.272)/(g2^9*y) + (2*g2^5*t^7.372)/(g1*y) + (2*g1*g2^9*t^7.372)/y + (2*g2^2*t^7.678)/y + (3*t^7.983)/(g1*g2^5*y) + (3*g1*t^7.983)/(g2*y) + t^8.289/(g1^2*g2^12*y) + (3*t^8.289)/(g2^8*y) + (g1^2*t^8.289)/(g2^4*y) + t^8.594/(g1*g2^15*y) + (g1*t^8.594)/(g2^11*y) + t^8.9/(g2^18*y) - (t^4.322*y)/g2^2 - g2^4*t^6.356*y - (t^6.661*y)/(g1*g2^3) - g1*g2*t^6.661*y - (t^7.272*y)/(g1*g2^13) - (g1*t^7.272*y)/g2^9 + (2*g2^5*t^7.372*y)/g1 + 2*g1*g2^9*t^7.372*y + 2*g2^2*t^7.678*y + (3*t^7.983*y)/(g1*g2^5) + (3*g1*t^7.983*y)/g2 + (t^8.289*y)/(g1^2*g2^12) + (3*t^8.289*y)/g2^8 + (g1^2*t^8.289*y)/g2^4 + (t^8.594*y)/(g1*g2^15) + (g1*t^8.594*y)/g2^11 + (t^8.9*y)/g2^18 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
46579 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6848 | 0.8448 | 0.8106 | [M:[0.9816, 0.9816, 1.1193, 0.7798, 0.7798], q:[0.578, 0.4404], qb:[0.4404, 0.7798], phi:[0.4404]] | 2*t^2.339 + t^2.642 + 2*t^2.945 + t^3.358 + 3*t^3.963 + t^4.073 + 2*t^4.376 + 3*t^4.679 + t^4.789 + 2*t^4.982 + 5*t^5.284 + 2*t^5.697 + 3*t^5.89 - 4*t^6. - t^4.321/y - t^4.321*y | detail |