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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58005 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{3}\phi_{1}^{3}$ | 1.4532 | 1.6401 | 0.8861 | [X:[1.3357], M:[1.0035, 0.9895, 1.0035], q:[0.4983, 0.5052], qb:[0.4983, 0.5052], phi:[0.3322]] | [X:[[0, 0, 2]], M:[[0, 0, 3], [0, 0, -9], [0, 0, 3]], q:[[-1, 0, -3], [0, -1, 9]], qb:[[1, 0, 0], [0, 1, 0]], phi:[[0, 0, -1]]] | 3 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{3}$ | ${}$ | -4 | t^2.97 + 4*t^3.01 + t^3.99 + 3*t^4.01 + t^4.03 + t^4.98 + 2*t^5. + t^5.02 + 2*t^5.5 + 2*t^5.52 + t^5.94 + 2*t^5.98 - 4*t^6. + 8*t^6.02 + 2*t^6.5 + 2*t^6.52 + t^6.95 + t^6.98 + 2*t^7. + 10*t^7.02 + 4*t^7.04 + 2*t^7.47 + 2*t^7.54 + t^7.95 + t^7.97 + 5*t^7.99 + 10*t^8.01 + 6*t^8.03 + t^8.06 - 4*t^8.49 + 2*t^8.51 + 6*t^8.53 + t^8.91 + 2*t^8.95 - 2*t^8.97 + 7*t^8.99 + t^8.99/y^2 - t^4./y - t^4.99/y - t^6.97/y - (4*t^7.01)/y - t^7.96/y - (4*t^8.)/y + (3*t^8.98)/y - t^4.*y - t^4.99*y - t^6.97*y - 4*t^7.01*y - t^7.96*y - 4*t^8.*y + 3*t^8.98*y + t^8.99*y^2 | t^2.97/g3^9 + (g2*t^3.01)/(g1*g3^3) + 2*g3^3*t^3.01 + (g1*g3^9*t^3.01)/g2 + t^3.99/g3^4 + (g2*t^4.01)/(g1*g3^4) + g3^2*t^4.01 + (g1*g3^8*t^4.01)/g2 + g3^8*t^4.03 + t^4.98/g3^5 + (g2*t^5.)/(g1*g3^5) + (g1*g3^7*t^5.)/g2 + g3^7*t^5.02 + (g1^2*g2*t^5.5)/g3 + (g3^2*t^5.5)/(g1^2*g2) + (g1*g2^2*t^5.52)/g3 + (g3^14*t^5.52)/(g1*g2^2) + t^5.94/g3^18 + (2*t^5.98)/g3^6 - 4*t^6. + (g2*t^6.02)/g1 + (g2^2*t^6.02)/(g1^2*g3^6) + 4*g3^6*t^6.02 + (g1*g3^12*t^6.02)/g2 + (g1^2*g3^18*t^6.02)/g2^2 + (g1^2*g2*t^6.5)/g3^2 + (g3*t^6.5)/(g1^2*g2) + (g1*g2^2*t^6.52)/g3^2 + (g3^13*t^6.52)/(g1*g2^2) + t^6.95/g3^13 + t^6.98/g3^7 + (g2*t^7.)/(g1*g3^7) + (g1*g3^5*t^7.)/g2 + (g2^2*t^7.02)/(g1^2*g3^7) + (2*g2*t^7.02)/(g1*g3) + 4*g3^5*t^7.02 + (2*g1*g3^11*t^7.02)/g2 + (g1^2*g3^17*t^7.02)/g2^2 + (g2*g3^5*t^7.04)/g1 + 2*g3^11*t^7.04 + (g1*g3^17*t^7.04)/g2 + t^7.47/(g1^3*g3^12) + (g1^3*t^7.47)/g3^3 + t^7.49/(g1^2*g2) - (g1*g2^2*t^7.49)/g3^9 + (g1^2*g2*t^7.49)/g3^3 - (g3^6*t^7.49)/(g1*g2^2) + (g1*g2^2*t^7.52)/g3^3 - g1^2*g2*g3^3*t^7.52 - (g3^6*t^7.52)/(g1^2*g2) + (g3^12*t^7.52)/(g1*g2^2) + (g2^3*t^7.54)/g3^3 + (g3^24*t^7.54)/g2^3 + t^7.95/g3^14 + t^7.97/g3^8 + (2*g2*t^7.99)/(g1*g3^8) + t^7.99/g3^2 + (2*g1*g3^4*t^7.99)/g2 + (2*g2^2*t^8.01)/(g1^2*g3^8) + (g2*t^8.01)/(g1*g3^2) + 4*g3^4*t^8.01 + (g1*g3^10*t^8.01)/g2 + (2*g1^2*g3^16*t^8.01)/g2^2 + (2*g2*g3^4*t^8.03)/g1 + 2*g3^10*t^8.03 + (2*g1*g3^16*t^8.03)/g2 + g3^16*t^8.06 - (g1*g2^2*t^8.49)/g3^10 - t^8.49/(g1^3*g3^7) - g1^3*g3^2*t^8.49 - (g3^5*t^8.49)/(g1*g2^2) - (g2^3*t^8.51)/g3^10 + (g1*g2^2*t^8.51)/g3^4 + t^8.51/(g1^3*g3) + g1^3*g3^8*t^8.51 + (g3^11*t^8.51)/(g1*g2^2) - (g3^17*t^8.51)/g2^3 + (g2^3*t^8.53)/g3^4 + g1*g2^2*g3^2*t^8.53 + g1^2*g2*g3^8*t^8.53 + (g3^11*t^8.53)/(g1^2*g2) + (g3^17*t^8.53)/(g1*g2^2) + (g3^23*t^8.53)/g2^3 + t^8.91/g3^27 + (2*t^8.95)/g3^15 - (2*t^8.97)/g3^9 + (2*g2*t^8.99)/(g1*g3^9) + (3*t^8.99)/g3^3 + (2*g1*g3^3*t^8.99)/g2 + t^8.99/(g3^3*y^2) - t^4./(g3*y) - t^4.99/(g3^2*y) - t^6.97/(g3^10*y) - (g2*t^7.01)/(g1*g3^4*y) - (2*g3^2*t^7.01)/y - (g1*g3^8*t^7.01)/(g2*y) - t^7.96/(g3^11*y) - (g2*t^8.)/(g1*g3^5*y) - (2*g3*t^8.)/y - (g1*g3^7*t^8.)/(g2*y) + (g1*t^8.98)/(g2*y) + (g2*t^8.98)/(g1*g3^12*y) + t^8.98/(g3^6*y) - (t^4.*y)/g3 - (t^4.99*y)/g3^2 - (t^6.97*y)/g3^10 - (g2*t^7.01*y)/(g1*g3^4) - 2*g3^2*t^7.01*y - (g1*g3^8*t^7.01*y)/g2 - (t^7.96*y)/g3^11 - (g2*t^8.*y)/(g1*g3^5) - 2*g3*t^8.*y - (g1*g3^7*t^8.*y)/g2 + (g1*t^8.98*y)/g2 + (g2*t^8.98*y)/(g1*g3^12) + (t^8.98*y)/g3^6 + (t^8.99*y^2)/g3^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
57311 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4539 | 1.6401 | 0.8865 | [X:[1.3403], M:[1.0104, 0.9687], q:[0.4948, 0.5157], qb:[0.4948, 0.5157], phi:[0.3299]] | t^2.906 + t^2.969 + 3*t^3.031 + t^3.958 + 3*t^4.021 + t^4.084 + t^4.948 + 2*t^5.01 + t^5.073 + 2*t^5.505 + 2*t^5.568 + t^5.812 + t^5.875 + 2*t^5.937 - t^6. - t^3.99/y - t^4.979/y - t^3.99*y - t^4.979*y | detail |