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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46097 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ | 0.5735 | 0.7428 | 0.772 | [M:[1.0, 1.0, 0.7206, 0.7206], q:[0.2151, 0.7849], qb:[0.7849, 0.4945], phi:[0.4302]] | [M:[[1, -1], [-1, 1], [-1, -7], [1, -9]], q:[[0, -1], [-1, 2]], qb:[[1, 0], [0, 7]], phi:[[0, -2]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{1}\tilde{q}_{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{3}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}q_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{3}q_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}^{4}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{2}$ | ${}M_{1}^{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{3}\tilde{q}_{2}$ | 1 | t^2.129 + 2*t^2.162 + 2*t^2.581 + 2*t^3. + t^3.419 + 2*t^4.257 + 2*t^4.29 + 3*t^4.324 + 3*t^4.71 + 4*t^4.743 + 2*t^5.129 + 6*t^5.162 + t^5.548 + 4*t^5.581 + t^6. + 2*t^6.386 + 2*t^6.419 + 2*t^6.452 + 4*t^6.485 + 2*t^6.838 + 4*t^6.871 + 6*t^6.905 + 2*t^7.257 + 5*t^7.29 + 10*t^7.324 + t^7.676 + 2*t^7.71 + 9*t^7.743 - t^8.129 + 2*t^8.162 + 3*t^8.515 + 2*t^8.614 + 5*t^8.647 + 2*t^8.967 - t^4.29/y - (2*t^6.452)/y - t^6.871/y + (2*t^7.29)/y + t^7.324/y + (3*t^7.71)/y + (4*t^7.743)/y + (4*t^8.129)/y + (5*t^8.162)/y + t^8.548/y + (6*t^8.581)/y - (3*t^8.614)/y - t^4.29*y - 2*t^6.452*y - t^6.871*y + 2*t^7.29*y + t^7.324*y + 3*t^7.71*y + 4*t^7.743*y + 4*t^8.129*y + 5*t^8.162*y + t^8.548*y + 6*t^8.581*y - 3*t^8.614*y | g2^6*t^2.129 + (g1*t^2.162)/g2^9 + t^2.162/(g1*g2^7) + (2*t^2.581)/g2^4 + (g1*t^3.)/g2 + (g2*t^3.)/g1 + g2^4*t^3.419 + 2*g2^12*t^4.257 + (g1*t^4.29)/g2^3 + t^4.29/(g1*g2) + (g1^2*t^4.324)/g2^18 + t^4.324/g2^16 + t^4.324/(g1^2*g2^14) + 3*g2^2*t^4.71 + (2*g1*t^4.743)/g2^13 + (2*t^4.743)/(g1*g2^11) + g1*g2^5*t^5.129 + (g2^7*t^5.129)/g1 + (g1^2*t^5.162)/g2^10 + (4*t^5.162)/g2^8 + t^5.162/(g1^2*g2^6) + g2^10*t^5.548 + (2*g1*t^5.581)/g2^5 + (2*t^5.581)/(g1*g2^3) - t^6. + (g1^2*t^6.)/g2^2 + (g2^2*t^6.)/g1^2 + 2*g2^18*t^6.386 + g1*g2^3*t^6.419 + (g2^5*t^6.419)/g1 + (g1^2*t^6.452)/g2^12 + t^6.452/(g1^2*g2^8) + (g1^3*t^6.485)/g2^27 + (g1*t^6.485)/g2^25 + t^6.485/(g1*g2^23) + t^6.485/(g1^3*g2^21) + 2*g2^8*t^6.838 + (2*g1*t^6.871)/g2^7 + (2*t^6.871)/(g1*g2^5) + (2*g1^2*t^6.905)/g2^22 + (2*t^6.905)/g2^20 + (2*t^6.905)/(g1^2*g2^18) + g1*g2^11*t^7.257 + (g2^13*t^7.257)/g1 + t^7.29/g1^2 + (g1^2*t^7.29)/g2^4 + (3*t^7.29)/g2^2 + (g1^3*t^7.324)/g2^19 + (4*g1*t^7.324)/g2^17 + (4*t^7.324)/(g1*g2^15) + t^7.324/(g1^3*g2^13) + g2^16*t^7.676 + g1*g2*t^7.71 + (g2^3*t^7.71)/g1 + (2*g1^2*t^7.743)/g2^14 + (5*t^7.743)/g2^12 + (2*t^7.743)/(g1^2*g2^10) + g1^2*g2^4*t^8.129 - 3*g2^6*t^8.129 + (g2^8*t^8.129)/g1^2 + (g1^3*t^8.162)/g2^11 + t^8.162/(g1^3*g2^5) + 3*g2^24*t^8.515 + (2*g1^2*t^8.581)/g2^6 - (4*t^8.581)/g2^4 + (2*t^8.581)/(g1^2*g2^2) + (g1^3*t^8.614)/g2^21 + t^8.614/(g1^3*g2^15) + (g1^4*t^8.647)/g2^36 + (g1^2*t^8.647)/g2^34 + t^8.647/g2^32 + t^8.647/(g1^2*g2^30) + t^8.647/(g1^4*g2^28) + 2*g2^14*t^8.967 - t^4.29/(g2^2*y) - (g1*t^6.452)/(g2^11*y) - t^6.452/(g1*g2^9*y) - t^6.871/(g2^6*y) + (g1*t^7.29)/(g2^3*y) + t^7.29/(g1*g2*y) + t^7.324/(g2^16*y) + (3*g2^2*t^7.71)/y + (2*g1*t^7.743)/(g2^13*y) + (2*t^7.743)/(g1*g2^11*y) + (2*g1*g2^5*t^8.129)/y + (2*g2^7*t^8.129)/(g1*y) + (g1^2*t^8.162)/(g2^10*y) + (3*t^8.162)/(g2^8*y) + t^8.162/(g1^2*g2^6*y) + (g2^10*t^8.548)/y + (3*g1*t^8.581)/(g2^5*y) + (3*t^8.581)/(g1*g2^3*y) - (g1^2*t^8.614)/(g2^20*y) - t^8.614/(g2^18*y) - t^8.614/(g1^2*g2^16*y) - (t^4.29*y)/g2^2 - (g1*t^6.452*y)/g2^11 - (t^6.452*y)/(g1*g2^9) - (t^6.871*y)/g2^6 + (g1*t^7.29*y)/g2^3 + (t^7.29*y)/(g1*g2) + (t^7.324*y)/g2^16 + 3*g2^2*t^7.71*y + (2*g1*t^7.743*y)/g2^13 + (2*t^7.743*y)/(g1*g2^11) + 2*g1*g2^5*t^8.129*y + (2*g2^7*t^8.129*y)/g1 + (g1^2*t^8.162*y)/g2^10 + (3*t^8.162*y)/g2^8 + (t^8.162*y)/(g1^2*g2^6) + g2^10*t^8.548*y + (3*g1*t^8.581*y)/g2^5 + (3*t^8.581*y)/(g1*g2^3) - (g1^2*t^8.614*y)/g2^20 - (t^8.614*y)/g2^18 - (t^8.614*y)/(g1^2*g2^16) |
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 |
---|---|---|---|---|---|---|---|---|---|
45944 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ | 0.6895 | 0.8743 | 0.7886 | [M:[0.6948, 0.6948, 0.6948, 0.6948], q:[0.4789, 0.8263], qb:[0.8263, 0.4789], phi:[0.3474]] | 5*t^2.084 + t^2.873 + 3*t^3.916 + 15*t^4.169 + 6*t^4.958 + t^5.747 + 6*t^6. - t^4.042/y - t^4.042*y | detail |